# Electronic Supplementary Material (ESI) for RSC Advances.
# This journal is © The Royal Society of Chemistry 2016

 
data_zhn20151023_7_0m 
 
_audit_creation_method            SHELXL-97 
_chemical_name_systematic 
; 
 ? 
; 
_chemical_name_common             ? 
_chemical_melting_point           ? 
_chemical_formula_moiety          ? 
_chemical_formula_sum 
 'B6 Cl K3 O10' 
_chemical_formula_weight          377.61 
 
loop_ 
 _atom_type_symbol 
 _atom_type_description 
 _atom_type_scat_dispersion_real 
 _atom_type_scat_dispersion_imag 
 _atom_type_scat_source 
 'B'  'B'   0.0013   0.0007 
 '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' 
 'Cl'  'Cl'   0.1484   0.1585 
 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' 
 'K'  'K'   0.2009   0.2494 
 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' 
 
_symmetry_cell_setting            Trigonal 
_symmetry_space_group_name_H-M    R3m 
 
loop_ 
 _symmetry_equiv_pos_as_xyz 
 'x, y, z' 
 '-y, x-y, z' 
 '-x+y, -x, z' 
 '-y, -x, z' 
 '-x+y, y, z' 
 'x, x-y, z' 
 'x+2/3, y+1/3, z+1/3' 
 '-y+2/3, x-y+1/3, z+1/3' 
 '-x+y+2/3, -x+1/3, z+1/3' 
 '-y+2/3, -x+1/3, z+1/3' 
 '-x+y+2/3, y+1/3, z+1/3' 
 'x+2/3, x-y+1/3, z+1/3' 
 'x+1/3, y+2/3, z+2/3' 
 '-y+1/3, x-y+2/3, z+2/3' 
 '-x+y+1/3, -x+2/3, z+2/3' 
 '-y+1/3, -x+2/3, z+2/3' 
 '-x+y+1/3, y+2/3, z+2/3' 
 'x+1/3, x-y+2/3, z+2/3' 
 
_cell_length_a                    10.0748(7) 
_cell_length_b                    10.0748(7) 
_cell_length_c                    8.8641(10) 
_cell_angle_alpha                 90.00 
_cell_angle_beta                  90.00 
_cell_angle_gamma                 120.00 
_cell_volume                      779.18(12) 
_cell_formula_units_Z             3 
_cell_measurement_temperature     296(2) 
_cell_measurement_reflns_used     1540 
_cell_measurement_theta_min       3.28 
_cell_measurement_theta_max       25.10 
 
_exptl_crystal_description        Block 
_exptl_crystal_colour             ? 
_exptl_crystal_size_max           ? 
_exptl_crystal_size_mid           ? 
_exptl_crystal_size_min           ? 
_exptl_crystal_density_meas       ? 
_exptl_crystal_density_diffrn     2.414 
_exptl_crystal_density_method     'not measured' 
_exptl_crystal_F_000              552 
_exptl_absorpt_coefficient_mu     1.614 
_exptl_absorpt_correction_type    ? 
_exptl_absorpt_correction_T_min   ? 
_exptl_absorpt_correction_T_max   ? 
_exptl_absorpt_process_details    ? 
 
_exptl_special_details 
; 
 ? 
; 
 
_diffrn_ambient_temperature       296(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 
_diffrn_measurement_method        ? 
_diffrn_detector_area_resol_mean  ? 
_diffrn_standards_number          ? 
_diffrn_standards_interval_count  ? 
_diffrn_standards_interval_time   ? 
_diffrn_standards_decay_%         ? 
_diffrn_reflns_number             1657 
_diffrn_reflns_av_R_equivalents   0.0266 
_diffrn_reflns_av_sigmaI/netI     0.0233 
_diffrn_reflns_limit_h_min        -12 
_diffrn_reflns_limit_h_max        12 
_diffrn_reflns_limit_k_min        -10 
_diffrn_reflns_limit_k_max        12 
_diffrn_reflns_limit_l_min        -10 
_diffrn_reflns_limit_l_max        10 
_diffrn_reflns_theta_min          3.28 
_diffrn_reflns_theta_max          25.10 
_reflns_number_total              360 
_reflns_number_gt                 360 
_reflns_threshold_expression      >2sigma(I) 
 
_computing_data_collection        ? 
_computing_cell_refinement        ? 
_computing_data_reduction         ? 
_computing_structure_solution     'SHELXS-97 (Sheldrick, 1990)' 
_computing_structure_refinement   'SHELXL-97 (Sheldrick, 1997)' 
_computing_molecular_graphics     ? 
_computing_publication_material   ? 
 
_refine_special_details 
; 
 Refinement of F² against ALL reflections.  The weighted R-factor wR and 
 goodness of fit S are based on F², conventional R-factors R are based 
 on F, with F set to zero for negative F². The threshold expression of 
 F² > 2sigma(F²) is used only for calculating R-factors(gt) etc. and is 
 not relevant to the choice of reflections for refinement.  R-factors based 
 on F² 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/[σ²(Fo²)+(0.0229P)²+0.2556P] where P=(Fo²+2Fc²)/3' 
_atom_sites_solution_primary      direct 
_atom_sites_solution_secondary    difmap 
_atom_sites_solution_hydrogens    none 
_refine_ls_hydrogen_treatment     none 
_refine_ls_extinction_method      SHELXL 
_refine_ls_extinction_coef        0.232(8) 
_refine_ls_extinction_expression 
 'Fc^*^=kFc[1+0.001xFc²λ³/sin(2θ)]^-1/4^' 
_refine_ls_abs_structure_details 
 'Flack H D (1983), Acta Cryst. A39, 876-881' 
_refine_ls_abs_structure_Flack    0.02(4) 
_refine_ls_number_reflns          360 
_refine_ls_number_parameters      41 
_refine_ls_number_restraints      1 
_refine_ls_R_factor_all           0.0146 
_refine_ls_R_factor_gt            0.0146 
_refine_ls_wR_factor_ref          0.0403 
_refine_ls_wR_factor_gt           0.0403 
_refine_ls_goodness_of_fit_ref    1.153 
_refine_ls_restrained_S_all       1.152 
_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 
Cl1 Cl 0.0000 0.0000 0.00384(16) 0.0281(3) Uani 1 6 d S . . 
K1 K 0.17902(3) 0.35804(7) 0.88208(3) 0.0196(2) Uani 1 2 d S . . 
O1 O 0.0000 0.0000 0.5519(3) 0.0058(6) Uani 1 6 d S . . 
O2 O 0.44433(8) 0.55567(8) 0.05487(19) 0.0121(4) Uani 1 2 d S . . 
O3 O 0.23350(13) 0.23429(12) 0.62309(16) 0.0121(3) Uani 1 1 d . . . 
B1 B 0.08740(13) 0.1748(3) 0.5444(3) 0.0081(5) Uani 1 2 d S . . 
B2 B 0.3004(3) 0.15020(16) 0.6590(3) 0.0089(6) Uani 1 2 d S . . 
 
 
_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 
Cl1 K1 3.2815(10) 8_554 ? 
Cl1 K1 3.2815(10) 7_444 ? 
Cl1 K1 3.2815(10) 9_454 ? 
Cl1 K1 3.3051(8) 2_554 ? 
Cl1 K1 3.3051(8) 1_554 ? 
Cl1 K1 3.3051(8) 3_554 ? 
K1 O3 2.7697(11) 8 ? 
K1 O3 2.7697(11) 12_455 ? 
K1 O3 2.7948(14) 5 ? 
K1 O3 2.7948(14) . ? 
K1 O2 2.8518(11) 3_566 ? 
K1 O2 2.8518(11) 1_556 ? 
K1 B2 3.1324(19) 8 ? 
K1 B2 3.1325(19) 7_455 ? 
K1 Cl1 3.2815(10) 13 ? 
K1 Cl1 3.3051(8) 1_556 ? 
K1 B1 3.394(3) . ? 
K1 B2 3.5147(19) 2 ? 
O1 B1 1.527(2) 2 ? 
O1 B1 1.527(2) . ? 
O1 B1 1.527(2) 3 ? 
O2 B2 1.376(4) 8_554 ? 
O2 B1 1.444(3) 15_554 ? 
O2 K1 2.8518(11) 2_664 ? 
O2 K1 2.8518(11) 1_554 ? 
O3 B2 1.3580(19) . ? 
O3 B1 1.4595(18) . ? 
O3 K1 2.7697(11) 15_554 ? 
B1 O2 1.444(3) 8 ? 
B1 O3 1.4595(18) 5 ? 
B2 O3 1.3580(19) 6 ? 
B2 O2 1.376(4) 15 ? 
B2 K1 3.1324(19) 15_554 ? 
B2 K1 3.1325(19) 13_544 ? 
B2 K1 3.5147(19) 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 
K1 Cl1 K1 90.58(3) 8_554 7_444 ? 
K1 Cl1 K1 90.57(3) 8_554 9_454 ? 
K1 Cl1 K1 90.57(3) 7_444 9_454 ? 
K1 Cl1 K1 164.20(5) 8_554 2_554 ? 
K1 Cl1 K1 78.394(6) 7_444 2_554 ? 
K1 Cl1 K1 78.394(6) 9_454 2_554 ? 
K1 Cl1 K1 78.394(6) 8_554 1_554 ? 
K1 Cl1 K1 164.20(5) 7_444 1_554 ? 
K1 Cl1 K1 78.394(6) 9_454 1_554 ? 
K1 Cl1 K1 109.88(2) 2_554 1_554 ? 
K1 Cl1 K1 78.395(6) 8_554 3_554 ? 
K1 Cl1 K1 78.395(6) 7_444 3_554 ? 
K1 Cl1 K1 164.20(5) 9_454 3_554 ? 
K1 Cl1 K1 109.88(2) 2_554 3_554 ? 
K1 Cl1 K1 109.88(2) 1_554 3_554 ? 
O3 K1 O3 150.91(6) 8 12_455 ? 
O3 K1 O3 124.78(5) 8 5 ? 
O3 K1 O3 76.019(19) 12_455 5 ? 
O3 K1 O3 76.019(19) 8 . ? 
O3 K1 O3 124.78(5) 12_455 . ? 
O3 K1 O3 49.60(5) 5 . ? 
O3 K1 O2 119.35(5) 8 3_566 ? 
O3 K1 O2 49.57(4) 12_455 3_566 ? 
O3 K1 O2 115.35(4) 5 3_566 ? 
O3 K1 O2 157.15(4) . 3_566 ? 
O3 K1 O2 49.57(4) 8 1_556 ? 
O3 K1 O2 119.35(5) 12_455 1_556 ? 
O3 K1 O2 157.15(5) 5 1_556 ? 
O3 K1 O2 115.35(4) . 1_556 ? 
O2 K1 O2 72.06(6) 3_566 1_556 ? 
O3 K1 B2 25.67(5) 8 8 ? 
O3 K1 B2 144.00(6) 12_455 8 ? 
O3 K1 B2 139.62(6) 5 8 ? 
O3 K1 B2 91.18(6) . 8 ? 
O2 K1 B2 98.09(6) 3_566 8 ? 
O2 K1 B2 26.04(6) 1_556 8 ? 
O3 K1 B2 144.01(6) 8 7_455 ? 
O3 K1 B2 25.67(5) 12_455 7_455 ? 
O3 K1 B2 91.18(6) 5 7_455 ? 
O3 K1 B2 139.62(6) . 7_455 ? 
O2 K1 B2 26.04(6) 3_566 7_455 ? 
O2 K1 B2 98.09(6) 1_556 7_455 ? 
B2 K1 B2 124.13(10) 8 7_455 ? 
O3 K1 Cl1 101.65(3) 8 13 ? 
O3 K1 Cl1 101.65(3) 12_455 13 ? 
O3 K1 Cl1 81.23(3) 5 13 ? 
O3 K1 Cl1 81.23(3) . 13 ? 
O2 K1 Cl1 79.09(4) 3_566 13 ? 
O2 K1 Cl1 79.09(4) 1_556 13 ? 
B2 K1 Cl1 83.76(4) 8 13 ? 
B2 K1 Cl1 83.77(4) 7_455 13 ? 
O3 K1 Cl1 81.16(3) 8 1_556 ? 
O3 K1 Cl1 81.16(3) 12_455 1_556 ? 
O3 K1 Cl1 84.44(3) 5 1_556 ? 
O3 K1 Cl1 84.44(3) . 1_556 ? 
O2 K1 Cl1 113.34(4) 3_566 1_556 ? 
O2 K1 Cl1 113.34(4) 1_556 1_556 ? 
B2 K1 Cl1 103.21(4) 8 1_556 ? 
B2 K1 Cl1 103.21(4) 7_455 1_556 ? 
Cl1 K1 Cl1 164.20(5) 13 1_556 ? 
O3 K1 B1 99.91(3) 8 . ? 
O3 K1 B1 99.91(3) 12_455 . ? 
O3 K1 B1 24.96(3) 5 . ? 
O3 K1 B1 24.96(3) . . ? 
O2 K1 B1 139.34(4) 3_566 . ? 
O2 K1 B1 139.34(4) 1_556 . ? 
B2 K1 B1 116.09(6) 8 . ? 
B2 K1 B1 116.09(6) 7_455 . ? 
Cl1 K1 B1 83.25(5) 13 . ? 
Cl1 K1 B1 80.95(5) 1_556 . ? 
O3 K1 B2 135.86(6) 8 2 ? 
O3 K1 B2 57.81(6) 12_455 2 ? 
O3 K1 B2 21.17(5) 5 2 ? 
O3 K1 B2 67.00(5) . 2 ? 
O2 K1 B2 103.55(6) 3_566 2 ? 
O2 K1 B2 173.76(5) 1_556 2 ? 
B2 K1 B2 157.89(10) 8 2 ? 
B2 K1 B2 77.599(15) 7_455 2 ? 
Cl1 K1 B2 95.84(4) 13 2 ? 
Cl1 K1 B2 72.31(4) 1_556 2 ? 
B1 K1 B2 42.32(5) . 2 ? 
B1 O1 B1 119.81(2) 2 . ? 
B1 O1 B1 119.81(3) 2 3 ? 
B1 O1 B1 119.81(3) . 3 ? 
B2 O2 B1 130.3(2) 8_554 15_554 ? 
B2 O2 K1 88.45(10) 8_554 2_664 ? 
B1 O2 K1 117.12(5) 15_554 2_664 ? 
B2 O2 K1 88.45(10) 8_554 1_554 ? 
B1 O2 K1 117.12(5) 15_554 1_554 ? 
K1 O2 K1 109.72(6) 2_664 1_554 ? 
B2 O3 B1 124.68(15) . . ? 
B2 O3 K1 92.26(12) . 15_554 ? 
B1 O3 K1 127.93(12) . 15_554 ? 
B2 O3 K1 110.82(15) . . ? 
B1 O3 K1 101.14(10) . . ? 
K1 O3 K1 96.85(4) 15_554 . ? 
O2 B1 O3 110.91(12) 8 . ? 
O2 B1 O3 110.91(12) 8 5 ? 
O3 B1 O3 106.87(19) . 5 ? 
O2 B1 O1 109.1(2) 8 . ? 
O3 B1 O1 109.53(14) . . ? 
O3 B1 O1 109.53(14) 5 . ? 
O2 B1 K1 135.33(14) 8 . ? 
O3 B1 K1 53.90(10) . . ? 
O3 B1 K1 53.90(10) 5 . ? 
O1 B1 K1 115.59(18) . . ? 
O3 B2 O3 121.4(2) 6 . ? 
O3 B2 O2 119.19(12) 6 15 ? 
O3 B2 O2 119.20(12) . 15 ? 
O3 B2 K1 146.09(19) 6 15_554 ? 
O3 B2 K1 62.07(9) . 15_554 ? 
O2 B2 K1 65.52(9) 15 15_554 ? 
O3 B2 K1 62.07(9) 6 13_544 ? 
O3 B2 K1 146.09(19) . 13_544 ? 
O2 B2 K1 65.51(9) 15 13_544 ? 
K1 B2 K1 96.23(8) 15_554 13_544 ? 
O3 B2 K1 48.01(11) 6 3 ? 
O3 B2 K1 132.33(16) . 3 ? 
O2 B2 K1 92.80(11) 15 3 ? 
K1 B2 K1 157.89(10) 15_554 3 ? 
K1 B2 K1 77.311(17) 13_544 3 ? 
O3 B2 K1 132.33(16) 6 . ? 
O3 B2 K1 48.01(11) . . ? 
O2 B2 K1 92.80(11) 15 . ? 
K1 B2 K1 77.311(17) 15_554 . ? 
K1 B2 K1 157.89(10) 13_544 . ? 
K1 B2 K1 100.66(8) 3 . ? 
 
_diffrn_measured_fraction_theta_max    1.000 
_diffrn_reflns_theta_full              25.10 
_diffrn_measured_fraction_theta_full   1.000 
_refine_diff_density_max    0.185 
_refine_diff_density_min   -0.280 
_refine_diff_density_rms    0.051 
