data_shelx _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common claringbullite _chemical_melting_point ? _chemical_formula_moiety ? _chemical_formula_sum 'CU4 O6 H6 CL1 F1' _chemical_formula_weight 410.61 loop_ _atom_type_symbol _atom_type_description _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source 'H' 'H' 0.0000 0.0000 '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' 'F' 'F' 0.0171 0.0103 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' 'Cl' 'Cl' 0.1484 0.1585 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' 'Cu' 'Cu' 0.3201 1.2651 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting ? _symmetry_space_group_name_H-M ? loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-y, x-y, z' '-x+y, -x, z' '-x, -y, z+1/2' 'y, -x+y, z+1/2' 'x-y, x, z+1/2' 'y, x, -z' 'x-y, -y, -z' '-x, -x+y, -z' '-y, -x, -z+1/2' '-x+y, y, -z+1/2' 'x, x-y, -z+1/2' '-x, -y, -z' 'y, -x+y, -z' 'x-y, x, -z' 'x, y, -z-1/2' '-y, x-y, -z-1/2' '-x+y, -x, -z-1/2' '-y, -x, z' '-x+y, y, z' 'x, x-y, z' 'y, x, z-1/2' 'x-y, -y, z-1/2' '-x, -x+y, z-1/2' _cell_length_a 6.66983(13) _cell_length_b 6.66983(13) _cell_length_c 9.1780(2) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 120.00 _cell_volume 353.594(14) _cell_formula_units_Z 4 _cell_measurement_temperature 293(2) _cell_measurement_reflns_used 2573 _cell_measurement_theta_min 2.2145 _cell_measurement_theta_max 31.9659 _exptl_crystal_description 'subhedral tabular crystal' _exptl_crystal_colour 'dark blue' _exptl_crystal_size_max 0.220 _exptl_crystal_size_mid 0.175 _exptl_crystal_size_min 0.065 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 3.857 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 392 _exptl_absorpt_coefficient_mu 12.245 _exptl_absorpt_correction_T_min 0.40218 _exptl_absorpt_correction_T_max 1.00000 _exptl_absorpt_correction_type 'multi-scan' _exptl_absorpt_process_details ? ; CrysAlisPro 1.171.39.23a (Rigaku Oxford Diffraction, 2015) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm. ; _exptl_special_details ; ? ; _diffrn_ambient_temperature 293(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 'Xcalibur EOS detector Agilent Technologies' _diffrn_measurement_method '1K CCD-based area detector' _diffrn_detector_area_resol_mean ? _diffrn_standards_number ? _diffrn_standards_interval_count 120 _diffrn_standards_interval_time ? _diffrn_standards_decay_% ? _diffrn_reflns_number 6946 _diffrn_reflns_av_R_equivalents 0.0500 _diffrn_reflns_av_sigmaI/netI 0.0149 _diffrn_reflns_limit_h_min -9 _diffrn_reflns_limit_h_max 9 _diffrn_reflns_limit_k_min -9 _diffrn_reflns_limit_k_max 9 _diffrn_reflns_limit_l_min -13 _diffrn_reflns_limit_l_max 13 _diffrn_reflns_theta_min 3.53 _diffrn_reflns_theta_max 32.04 _reflns_number_total 263 _reflns_number_gt 248 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'CrysAlisPro, Agilent Technologies, Version 1.171.35.19 (release 27-10-2011 CrysAlis171 .NET)' _computing_cell_refinement 'CrysAlisPro, Agilent Technologies, Version 1.171.35.19 (release 27-10-2011 CrysAlis171 .NET)' _computing_data_reduction 'CrysAlisPro, Agilent Technologies, Version 1.171.35.19 (release 27-10-2011 CrysAlis171 .NET)' _computing_structure_solution 'SHELXS-97 (Sheldrick, 2008)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 2008)' _computing_molecular_graphics 'Crystalmaker' _computing_publication_material ? _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. ; _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^)+(0.0254P)^2^+0.1978P] 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 mixed _refine_ls_extinction_method SHELXL _refine_ls_extinction_coef 0.314(11) _refine_ls_extinction_expression 'Fc^*^=kFc[1+0.001xFc^2^\l^3^/sin(2\q)]^-1/4^' _refine_ls_number_reflns 263 _refine_ls_number_parameters 23 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0186 _refine_ls_R_factor_gt 0.0171 _refine_ls_wR_factor_ref 0.0503 _refine_ls_wR_factor_gt 0.0494 _refine_ls_goodness_of_fit_ref 1.189 _refine_ls_restrained_S_all 1.189 _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_symetry_multiplicity _atom_site_calc_flag _atom_site_refinement_flags _atom_site_disorder_assembly _atom_site_disorder_group Cu1 Cu 0.37123(8) 0.74245(15) 0.2500 0.0113(3) Uani 0.33 4 d SP . . Cu2 Cu 0.5000 0.0000 0.0000 0.0150(2) Uani 1 4 d S . . Cl Cl 0.3333 0.6667 0.7500 0.0237(3) Uani 1 12 d S . . F F 0.0000 0.0000 0.2500 0.0203(7) Uani 1 12 d S . . O O 0.20205(11) 0.4041(2) 0.09135(14) 0.0118(3) Uani 1 2 d S . . H H 0.140(3) 0.281(6) 0.128(3) 0.034(9) Uiso 1 2 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 Cu1 0.0104(3) 0.0165(4) 0.0089(4) 0.000 0.000 0.0083(2) Cu2 0.0103(2) 0.0102(2) 0.0246(3) 0.00543(11) 0.00271(6) 0.00509(12) Cl 0.0270(4) 0.0270(4) 0.0171(6) 0.000 0.000 0.0135(2) F 0.0163(9) 0.0163(9) 0.0284(18) 0.000 0.000 0.0081(5) O 0.0102(4) 0.0105(6) 0.0148(6) 0.0019(5) 0.0010(2) 0.0053(3) _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 Cu1 Cu1 0.7582(15) 2_665 ? Cu1 Cu1 0.7582(15) 3_565 ? Cu1 O 1.9870(13) 3_565 ? Cu1 O 1.9870(13) 18_566 ? Cu1 O 1.9870(13) 17_666 ? Cu1 O 1.9870(13) 2_665 ? Cu1 O 2.4372(15) . ? Cu1 O 2.4372(15) 16_556 ? Cu1 Cu2 2.7346(5) 4_665 ? Cu1 Cu2 2.7346(5) 1_565 ? Cu2 O 1.9468(7) 3 ? Cu2 O 1.9468(7) 15_655 ? Cu2 O 1.9468(7) 14 ? Cu2 O 1.9468(7) 2_655 ? Cu2 Cu1 2.7346(5) 13_665 ? Cu2 Cu1 2.7346(5) 1_545 ? O Cu2 1.9468(7) 2 ? O Cu2 1.9468(7) 3_665 ? O Cu1 1.9870(13) 2_665 ? O Cu1 1.9870(13) 3_565 ? 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 Cu1 Cu1 Cu1 60.0 2_665 3_565 ? Cu1 Cu1 O 79.00(2) 2_665 3_565 ? Cu1 Cu1 O 118.05(4) 3_565 3_565 ? Cu1 Cu1 O 79.00(2) 2_665 18_566 ? Cu1 Cu1 O 118.05(4) 3_565 18_566 ? O Cu1 O 94.24(8) 3_565 18_566 ? Cu1 Cu1 O 118.05(4) 2_665 17_666 ? Cu1 Cu1 O 79.00(2) 3_565 17_666 ? O Cu1 O 161.43(6) 3_565 17_666 ? O Cu1 O 82.76(7) 18_566 17_666 ? Cu1 Cu1 O 118.05(4) 2_665 2_665 ? Cu1 Cu1 O 79.00(2) 3_565 2_665 ? O Cu1 O 82.76(7) 3_565 2_665 ? O Cu1 O 161.43(6) 18_566 2_665 ? O Cu1 O 94.24(8) 17_666 2_665 ? Cu1 Cu1 O 46.01(2) 2_665 . ? Cu1 Cu1 O 46.01(2) 3_565 . ? O Cu1 O 72.03(5) 3_565 . ? O Cu1 O 124.55(4) 18_566 . ? O Cu1 O 124.55(4) 17_666 . ? O Cu1 O 72.03(5) 2_665 . ? Cu1 Cu1 O 46.01(2) 2_665 16_556 ? Cu1 Cu1 O 46.01(2) 3_565 16_556 ? O Cu1 O 124.55(4) 3_565 16_556 ? O Cu1 O 72.03(5) 18_566 16_556 ? O Cu1 O 72.04(5) 17_666 16_556 ? O Cu1 O 124.55(4) 2_665 16_556 ? O Cu1 O 73.37(7) . 16_556 ? Cu1 Cu1 Cu2 118.108(13) 2_665 4_665 ? Cu1 Cu1 Cu2 118.108(13) 3_565 4_665 ? O Cu1 Cu2 121.81(5) 3_565 4_665 ? O Cu1 Cu2 45.36(2) 18_566 4_665 ? O Cu1 Cu2 45.36(2) 17_666 4_665 ? O Cu1 Cu2 121.81(5) 2_665 4_665 ? O Cu1 Cu2 159.64(4) . 4_665 ? O Cu1 Cu2 86.27(3) 16_556 4_665 ? Cu1 Cu1 Cu2 118.108(13) 2_665 1_565 ? Cu1 Cu1 Cu2 118.108(13) 3_565 1_565 ? O Cu1 Cu2 45.36(2) 3_565 1_565 ? O Cu1 Cu2 121.81(5) 18_566 1_565 ? O Cu1 Cu2 121.81(5) 17_666 1_565 ? O Cu1 Cu2 45.36(2) 2_665 1_565 ? O Cu1 Cu2 86.27(3) . 1_565 ? O Cu1 Cu2 159.64(4) 16_556 1_565 ? Cu2 Cu1 Cu2 114.08(3) 4_665 1_565 ? O Cu2 O 180.00(8) 3 15_655 ? O Cu2 O 95.14(8) 3 14 ? O Cu2 O 84.86(8) 15_655 14 ? O Cu2 O 84.86(8) 3 2_655 ? O Cu2 O 95.14(8) 15_655 2_655 ? O Cu2 O 180.00(7) 14 2_655 ? O Cu2 Cu1 133.43(4) 3 13_665 ? O Cu2 Cu1 46.57(4) 15_655 13_665 ? O Cu2 Cu1 46.57(4) 14 13_665 ? O Cu2 Cu1 133.43(4) 2_655 13_665 ? O Cu2 Cu1 46.57(4) 3 1_545 ? O Cu2 Cu1 133.43(4) 15_655 1_545 ? O Cu2 Cu1 133.43(4) 14 1_545 ? O Cu2 Cu1 46.57(4) 2_655 1_545 ? Cu1 Cu2 Cu1 180.00(6) 13_665 1_545 ? Cu2 O Cu2 117.85(7) 2 3_665 ? Cu2 O Cu1 88.07(4) 2 2_665 ? Cu2 O Cu1 107.05(6) 3_665 2_665 ? Cu2 O Cu1 107.05(6) 2 3_565 ? Cu2 O Cu1 88.07(4) 3_665 3_565 ? Cu1 O Cu1 22.00(5) 2_665 3_565 ? Cu2 O Cu1 91.67(4) 2 . ? Cu2 O Cu1 91.67(4) 3_665 . ? Cu1 O Cu1 15.94(3) 2_665 . ? Cu1 O Cu1 15.94(3) 3_565 . ? _diffrn_measured_fraction_theta_max 0.985 _diffrn_reflns_theta_full 32.04 _diffrn_measured_fraction_theta_full 0.985 _refine_diff_density_max 0.556 _refine_diff_density_min -0.356 _refine_diff_density_rms 0.117