data_dienerite _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common 'dienerite' _chemical_melting_point ? _chemical_formula_moiety ? _chemical_formula_sum 'As Ni3' _chemical_formula_weight 251.05 loop_ _atom_type_symbol _atom_type_description _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source 'Ni' 'Ni' 0.3393 1.1124 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' 'As' 'As' 0.0499 2.0058 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting 'cubic' _symmetry_space_group_name_H-M 'I-43d' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' 'x, -y, -z+1/2' '-x, -y+1/2, z' '-x, y+1/2, -z+1/2' 'y+1/4, -x+3/4, -z+1/4' '-y+1/4, -x+3/4, z+3/4' '-y+3/4, x+3/4, -z+1/4' 'y+3/4, x+3/4, z+3/4' 'y, z, x' '-y, -z+1/2, x' 'y, -z, -x+1/2' '-y, z+1/2, -x+1/2' 'z+1/4, -y+3/4, -x+1/4' 'z+1/4, y+1/4, x+1/4' '-z+3/4, y+3/4, -x+1/4' '-z+3/4, -y+1/4, x+1/4' 'z, x, y' '-z+1/2, x, -y' '-z, -x+1/2, y' 'z+1/2, -x+1/2, -y' 'x+3/4, z+3/4, y+3/4' 'x+3/4, -z+1/4, -y+3/4' '-x+3/4, z+3/4, -y+1/4' '-x+1/4, -z+3/4, y+3/4' 'x+1/2, y+1/2, z+1/2' 'x+1/2, -y+1/2, -z+1' '-x+1/2, -y+1, z+1/2' '-x+1/2, y+1, -z+1' 'y+3/4, -x+5/4, -z+3/4' '-y+3/4, -x+5/4, z+5/4' '-y+5/4, x+5/4, -z+3/4' 'y+5/4, x+5/4, z+5/4' 'y+1/2, z+1/2, x+1/2' '-y+1/2, -z+1, x+1/2' 'y+1/2, -z+1/2, -x+1' '-y+1/2, z+1, -x+1' 'z+3/4, -y+5/4, -x+3/4' 'z+3/4, y+3/4, x+3/4' '-z+5/4, y+5/4, -x+3/4' '-z+5/4, -y+3/4, x+3/4' 'z+1/2, x+1/2, y+1/2' '-z+1, x+1/2, -y+1/2' '-z+1/2, -x+1, y+1/2' 'z+1, -x+1, -y+1/2' 'x+5/4, z+5/4, y+5/4' 'x+5/4, -z+3/4, -y+5/4' '-x+5/4, z+5/4, -y+3/4' '-x+3/4, -z+5/4, y+5/4' _cell_length_a 9.6206(9) _cell_length_b 9.6206(9) _cell_length_c 9.6206(9) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 890.44(14) _cell_formula_units_Z 16 _cell_measurement_temperature 298(2) _cell_measurement_reflns_used 356 _cell_measurement_theta_min 9.5 _cell_measurement_theta_max 21.1 _exptl_crystal_description block _exptl_crystal_colour black _exptl_crystal_size_max 0.015 _exptl_crystal_size_mid 0.012 _exptl_crystal_size_min 0.010 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 7.491 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 1872 _exptl_absorpt_coefficient_mu 39.405 _exptl_absorpt_correction_type 'multi-scan' _exptl_absorpt_correction_T_min 0.0469 _exptl_absorpt_correction_T_max 0.0469 _exptl_absorpt_process_details '(ABSPACK; Bruker Inc., 2015)' _exptl_special_details ; ? ; _diffrn_ambient_temperature 298(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 D8 Venture' _diffrn_measurement_method '\w scans' _diffrn_detector_area_resol_mean ? _diffrn_standards_number ? _diffrn_standards_interval_count . _diffrn_standards_interval_time . _diffrn_standards_decay_% ? _diffrn_reflns_number 1933 _diffrn_reflns_av_R_equivalents 0.0558 _diffrn_reflns_av_sigmaI/netI 0.0469 _diffrn_reflns_limit_h_min -9 _diffrn_reflns_limit_h_max 15 _diffrn_reflns_limit_k_min -12 _diffrn_reflns_limit_k_max 12 _diffrn_reflns_limit_l_min -4 _diffrn_reflns_limit_l_max 15 _diffrn_reflns_theta_min 5.19 _diffrn_reflns_theta_max 34.74 _reflns_number_total 327 _reflns_number_gt 297 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'APEX3 (Bruker Inc., 2016)' _computing_cell_refinement 'APEX3 (Bruker Inc., 2016)' _computing_data_reduction 'APEX3 (Bruker Inc., 2016)' _computing_structure_solution 'SHELXS-97 (Sheldrick, 2008)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 2008)' _computing_molecular_graphics 'DIAMOND (Brandenburg, 2001)' _computing_publication_material 'SHELXL-97 (Sheldrick, 2008)' _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^)+(0.0118P)^2^+0.0000P] where P=(Fo^2^+2Fc^2^)/3' _atom_sites_solution_primary direct _atom_sites_solution_secondary difmap _atom_sites_solution_hydrogens . _refine_ls_hydrogen_treatment . _refine_ls_extinction_method SHELXL _refine_ls_extinction_coef 0.00097(17) _refine_ls_extinction_expression 'Fc^*^=kFc[1+0.001xFc^2^\l^3^/sin(2\q)]^-1/4^' _refine_ls_abs_structure_details 'Flack H D (1983), Acta Cryst. A39, 876-881' _refine_ls_abs_structure_Flack 0.13(7) _refine_ls_number_reflns 327 _refine_ls_number_parameters 14 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0424 _refine_ls_R_factor_gt 0.0353 _refine_ls_wR_factor_ref 0.0616 _refine_ls_wR_factor_gt 0.0595 _refine_ls_goodness_of_fit_ref 1.143 _refine_ls_restrained_S_all 1.143 _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 Ni Ni -0.02902(8) 0.12026(8) 0.18792(8) 0.0139(2) Uani 1 1 d . . . As As -0.02971(7) -0.02971(7) -0.02971(7) 0.0119(3) Uani 1 3 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 Ni 0.0132(4) 0.0091(4) 0.0195(5) -0.0007(3) 0.0047(3) -0.0002(3) As 0.0119(3) 0.0119(3) 0.0119(3) 0.0000(2) 0.0000(2) 0.0000(2) _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 Ni As 2.4159(9) 30_444 ? Ni As 2.5427(12) . ? Ni Ni 2.5580(16) 3 ? Ni Ni 2.6041(16) 2 ? Ni As 2.6031(12) 32_444 ? Ni Ni 2.6080(13) 23_445 ? Ni Ni 2.6080(13) 48_444 ? Ni Ni 2.6157(13) 9 ? Ni Ni 2.6157(13) 17 ? Ni Ni 2.9209(5) 44_445 ? Ni Ni 2.9209(5) 10 ? As Ni 2.4159(9) 23_445 ? As Ni 2.4159(9) 37_444 ? As Ni 2.4159(9) 6_544 ? As Ni 2.5427(12) 17 ? As Ni 2.5427(12) 9 ? As Ni 2.6031(12) 38_444 ? As Ni 2.6031(12) 8_444 ? As Ni 2.6031(12) 21_444 ? 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 As Ni As 117.68(4) 30_444 . ? As Ni Ni 63.04(4) 30_444 3 ? As Ni Ni 123.66(2) . 3 ? As Ni Ni 120.34(4) 30_444 2 ? As Ni Ni 82.73(4) . 2 ? Ni Ni Ni 150.13(3) 3 2 ? As Ni As 116.85(3) 30_444 32_444 ? As Ni As 108.10(3) . 32_444 ? Ni Ni As 55.81(3) 3 32_444 ? Ni Ni As 105.88(2) 2 32_444 ? As Ni Ni 85.14(5) 30_444 23_445 ? As Ni Ni 55.93(3) . 23_445 ? Ni Ni Ni 144.19(6) 3 23_445 ? Ni Ni Ni 60.049(19) 2 23_445 ? As Ni Ni 157.95(5) 32_444 23_445 ? As Ni Ni 60.67(4) 30_444 48_444 ? As Ni Ni 115.48(4) . 48_444 ? Ni Ni Ni 111.35(4) 3 48_444 ? Ni Ni Ni 60.049(19) 2 48_444 ? As Ni Ni 130.64(5) 32_444 48_444 ? Ni Ni Ni 59.90(4) 23_445 48_444 ? As Ni Ni 111.29(5) 30_444 9 ? As Ni Ni 59.045(18) . 9 ? Ni Ni Ni 68.74(2) 3 9 ? Ni Ni Ni 125.95(4) 2 9 ? As Ni Ni 59.840(18) 32_444 9 ? Ni Ni Ni 112.64(3) 23_445 9 ? Ni Ni Ni 168.21(5) 48_444 9 ? As Ni Ni 171.29(5) 30_444 17 ? As Ni Ni 59.045(18) . 17 ? Ni Ni Ni 111.20(3) 3 17 ? Ni Ni Ni 68.05(3) 2 17 ? As Ni Ni 59.840(18) 32_444 17 ? Ni Ni Ni 98.18(4) 23_445 17 ? Ni Ni Ni 127.92(5) 48_444 17 ? Ni Ni Ni 60.0 9 17 ? As Ni Ni 130.82(4) 30_444 44_445 ? As Ni Ni 110.58(3) . 44_445 ? Ni Ni Ni 97.89(5) 3 44_445 ? Ni Ni Ni 56.16(3) 2 44_445 ? As Ni Ni 51.48(3) 32_444 44_445 ? Ni Ni Ni 116.07(3) 23_445 44_445 ? Ni Ni Ni 90.95(3) 48_444 44_445 ? Ni Ni Ni 100.75(4) 9 44_445 ? Ni Ni Ni 54.70(4) 17 44_445 ? As Ni Ni 57.46(3) 30_444 10 ? As Ni Ni 76.67(3) . 10 ? Ni Ni Ni 56.57(3) 3 10 ? Ni Ni Ni 152.77(5) 2 10 ? As Ni Ni 97.40(3) 32_444 10 ? Ni Ni Ni 93.37(5) 23_445 10 ? Ni Ni Ni 113.79(4) 48_444 10 ? Ni Ni Ni 55.78(4) 9 10 ? Ni Ni Ni 114.13(4) 17 10 ? Ni Ni Ni 148.87(4) 44_445 10 ? Ni As Ni 117.860(15) 23_445 37_444 ? Ni As Ni 117.860(15) 23_445 6_544 ? Ni As Ni 117.860(15) 37_444 6_544 ? Ni As Ni 105.50(3) 23_445 17 ? Ni As Ni 122.46(4) 37_444 17 ? Ni As Ni 63.40(3) 6_544 17 ? Ni As Ni 122.46(4) 23_445 9 ? Ni As Ni 63.40(3) 37_444 9 ? Ni As Ni 105.50(3) 6_544 9 ? Ni As Ni 61.91(4) 17 9 ? Ni As Ni 63.40(3) 23_445 . ? Ni As Ni 105.50(3) 37_444 . ? Ni As Ni 122.46(4) 6_544 . ? Ni As Ni 61.91(4) 17 . ? Ni As Ni 61.91(4) 9 . ? Ni As Ni 116.50(5) 23_445 38_444 ? Ni As Ni 61.15(3) 37_444 38_444 ? Ni As Ni 71.07(2) 6_544 38_444 ? Ni As Ni 128.49(3) 17 38_444 ? Ni As Ni 112.01(3) 9 38_444 ? Ni As Ni 165.65(4) . 38_444 ? Ni As Ni 71.07(2) 23_445 8_444 ? Ni As Ni 116.50(5) 37_444 8_444 ? Ni As Ni 61.15(3) 6_544 8_444 ? Ni As Ni 112.01(3) 17 8_444 ? Ni As Ni 165.65(4) 9 8_444 ? Ni As Ni 128.49(3) . 8_444 ? Ni As Ni 60.32(4) 38_444 8_444 ? Ni As Ni 61.15(3) 23_445 21_444 ? Ni As Ni 71.07(2) 37_444 21_444 ? Ni As Ni 116.50(5) 6_544 21_444 ? Ni As Ni 165.65(4) 17 21_444 ? Ni As Ni 128.49(3) 9 21_444 ? Ni As Ni 112.01(3) . 21_444 ? Ni As Ni 60.32(4) 38_444 21_444 ? Ni As Ni 60.32(4) 8_444 21_444 ? _diffrn_measured_fraction_theta_max 1.000 _diffrn_reflns_theta_full 34.74 _diffrn_measured_fraction_theta_full 1.000 _refine_diff_density_max 0.820 _refine_diff_density_min -1.163 _refine_diff_density_rms 0.225