 
data_3
 
_audit_creation_method            'SHELXL-2014/7'
_shelx_SHELXL_version_number      '2014/7'
_chemical_name_systematic         ?
_chemical_name_common             ?
_chemical_melting_point           ?
_chemical_formula_moiety          ?
_chemical_formula_sum
 'C48 H0 B24 F96 N24' 
_chemical_formula_weight          2996.16

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'
 'B'  'B'   0.0013   0.0007
 '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'
 'F'  'F'   0.0171   0.0103
 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'
 
_space_group_crystal_system       cubic
_space_group_IT_number            226
_space_group_name_H-M_alt         'F m -3 c'
_space_group_name_Hall            '-F 4c 2 3'
 
_shelx_space_group_comment
;
The symmetry employed for this shelxl refinement is uniquely defined
by the following loop, which should always be used as a source of
symmetry information in preference to the above space-group names.
They are only intended as comments.
;
 
loop_
 _space_group_symop_operation_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+1/2, x+1/2, -z+1/2'
 '-y+1/2, -x+1/2, -z+1/2'
 'y+1/2, -x+1/2, z+1/2'
 '-y+1/2, x+1/2, z+1/2'
 'x+1/2, z+1/2, -y+1/2'
 '-x+1/2, z+1/2, y+1/2'
 '-x+1/2, -z+1/2, -y+1/2'
 'x+1/2, -z+1/2, y+1/2'
 'z+1/2, y+1/2, -x+1/2'
 'z+1/2, -y+1/2, x+1/2'
 '-z+1/2, y+1/2, x+1/2'
 '-z+1/2, -y+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'
 '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+1/2, x+1, -z+1'
 '-y+1/2, -x+1, -z+1'
 'y+1/2, -x+1, z+1'
 '-y+1/2, x+1, z+1'
 'x+1/2, z+1, -y+1'
 '-x+1/2, z+1, y+1'
 '-x+1/2, -z+1, -y+1'
 'x+1/2, -z+1, y+1'
 'z+1/2, y+1, -x+1'
 'z+1/2, -y+1, x+1'
 '-z+1/2, y+1, x+1'
 '-z+1/2, -y+1, -x+1'
 '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, x+1/2, -z+1'
 '-y+1, -x+1/2, -z+1'
 'y+1, -x+1/2, z+1'
 '-y+1, x+1/2, z+1'
 'x+1, z+1/2, -y+1'
 '-x+1, z+1/2, y+1'
 '-x+1, -z+1/2, -y+1'
 'x+1, -z+1/2, y+1'
 'z+1, y+1/2, -x+1'
 'z+1, -y+1/2, x+1'
 '-z+1, y+1/2, x+1'
 '-z+1, -y+1/2, -x+1'
 '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, x+1, -z+1/2'
 '-y+1, -x+1, -z+1/2'
 'y+1, -x+1, z+1/2'
 '-y+1, x+1, z+1/2'
 'x+1, z+1, -y+1/2'
 '-x+1, z+1, y+1/2'
 '-x+1, -z+1, -y+1/2'
 'x+1, -z+1, y+1/2'
 'z+1, y+1, -x+1/2'
 'z+1, -y+1, x+1/2'
 '-z+1, y+1, x+1/2'
 '-z+1, -y+1, -x+1/2'
 '-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-1/2, -x-1/2, z-1/2'
 'y-1/2, x-1/2, z-1/2'
 '-y-1/2, x-1/2, -z-1/2'
 'y-1/2, -x-1/2, -z-1/2'
 '-x-1/2, -z-1/2, y-1/2'
 'x-1/2, -z-1/2, -y-1/2'
 'x-1/2, z-1/2, y-1/2'
 '-x-1/2, z-1/2, -y-1/2'
 '-z-1/2, -y-1/2, x-1/2'
 '-z-1/2, y-1/2, -x-1/2'
 'z-1/2, -y-1/2, -x-1/2'
 'z-1/2, y-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'
 '-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-1/2, -x, z'
 'y-1/2, x, z'
 '-y-1/2, x, -z'
 'y-1/2, -x, -z'
 '-x-1/2, -z, y'
 'x-1/2, -z, -y'
 'x-1/2, z, y'
 '-x-1/2, z, -y'
 '-z-1/2, -y, x'
 '-z-1/2, y, -x'
 'z-1/2, -y, -x'
 'z-1/2, y, x'
 '-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, -x-1/2, z'
 'y, x-1/2, z'
 '-y, x-1/2, -z'
 'y, -x-1/2, -z'
 '-x, -z-1/2, y'
 'x, -z-1/2, -y'
 'x, z-1/2, y'
 '-x, z-1/2, -y'
 '-z, -y-1/2, x'
 '-z, y-1/2, -x'
 'z, -y-1/2, -x'
 'z, y-1/2, x'
 '-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, -x, z-1/2'
 'y, x, z-1/2'
 '-y, x, -z-1/2'
 'y, -x, -z-1/2'
 '-x, -z, y-1/2'
 'x, -z, -y-1/2'
 'x, z, y-1/2'
 '-x, z, -y-1/2'
 '-z, -y, x-1/2'
 '-z, y, -x-1/2'
 'z, -y, -x-1/2'
 'z, y, x-1/2'
 
_cell_length_a                    14.3006(4)
_cell_length_b                    14.3006(4)
_cell_length_c                    14.3006(4)
_cell_angle_alpha                 90
_cell_angle_beta                  90
_cell_angle_gamma                 90
_cell_volume                      2924.6(2)
_cell_formula_units_Z             1
_cell_measurement_temperature     358(2)
_cell_measurement_reflns_used     694
_cell_measurement_theta_min       2.8290
_cell_measurement_theta_max       27.445
 
_exptl_crystal_description        block
_exptl_crystal_colour             ?
_exptl_crystal_density_meas       ?
_exptl_crystal_density_method     ?
_exptl_crystal_density_diffrn     1.701          
_exptl_crystal_F_000              1440
_exptl_transmission_factor_min    ?
_exptl_transmission_factor_max    ?
_exptl_crystal_size_max           ?
_exptl_crystal_size_mid           ?
_exptl_crystal_size_min           ?
_exptl_absorpt_coefficient_mu     0.209
_shelx_estimated_absorpt_T_min    ?
_shelx_estimated_absorpt_T_max    ?
_exptl_absorpt_correction_type    ?
_exptl_absorpt_correction_T_min   ?
_exptl_absorpt_correction_T_max   ?
_exptl_absorpt_process_details    ?
_exptl_absorpt_special_details    ?
_diffrn_ambient_temperature       358(2)
_diffrn_radiation_wavelength      0.71073
_diffrn_radiation_type            MoK\a
_diffrn_source                    ?
_diffrn_measurement_device_type   'XtaLAB Synergy R, DW system, HyPix'
_diffrn_measurement_method        ?
_diffrn_detector_area_resol_mean  ?
_diffrn_reflns_number             950
_diffrn_reflns_av_unetI/netI      0.0059
_diffrn_reflns_av_R_equivalents   0.0078
_diffrn_reflns_limit_h_min        -18
_diffrn_reflns_limit_h_max        12
_diffrn_reflns_limit_k_min        -16
_diffrn_reflns_limit_k_max        7
_diffrn_reflns_limit_l_min        -17
_diffrn_reflns_limit_l_max        17
_diffrn_reflns_theta_min          2.849
_diffrn_reflns_theta_max          27.445
_diffrn_reflns_theta_full         25.242
_diffrn_measured_fraction_theta_max   0.988
_diffrn_measured_fraction_theta_full  1.000
_diffrn_reflns_Laue_measured_fraction_max    0.988
_diffrn_reflns_Laue_measured_fraction_full   1.000
_diffrn_reflns_point_group_measured_fraction_max   0.988
_diffrn_reflns_point_group_measured_fraction_full  1.000
_reflns_number_total              164
_reflns_number_gt                 151
_reflns_threshold_expression      'I > 2σ(I)'
_reflns_Friedel_coverage          0.000
_reflns_Friedel_fraction_max      .
_reflns_Friedel_fraction_full     .
 
_reflns_special_details
;
 Reflections were merged by SHELXL according to the crystal
 class for the calculation of statistics and refinement.
 
 _reflns_Friedel_fraction is defined as the number of unique
 Friedel pairs measured divided by the number that would be
 possible theoretically, ignoring centric projections and
 systematic absences.
;
 
_computing_data_collection        ?
_computing_cell_refinement        ?
_computing_data_reduction         ?
_computing_structure_solution     ?
_computing_structure_refinement 'SHELXL-2014/7 (Sheldrick, 2014)'
_computing_molecular_graphics     ?
_computing_publication_material   ?
_refine_special_details           ?
_refine_ls_structure_factor_coef  Fsqd
_refine_ls_matrix_type            full
_refine_ls_weighting_scheme       calc
_refine_ls_weighting_details
'w=1/[σ²(Fo²)+(0.4000P)²+5.0000P] where P=(Fo²+2Fc²)/3'
_atom_sites_solution_primary      ?
_atom_sites_solution_secondary    ?
_atom_sites_solution_hydrogens    .
_refine_ls_hydrogen_treatment     undef
_refine_ls_extinction_method      none
_refine_ls_extinction_coef        .
_refine_ls_number_reflns          164
_refine_ls_number_parameters      16
_refine_ls_number_restraints      2
_refine_ls_R_factor_all           0.1324
_refine_ls_R_factor_gt            0.1303
_refine_ls_wR_factor_ref          0.4938
_refine_ls_wR_factor_gt           0.4880
_refine_ls_goodness_of_fit_ref    1.228
_refine_ls_restrained_S_all       1.255
_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_site_symmetry_order  
 _atom_site_calc_flag
 _atom_site_refinement_flags_posn
 _atom_site_refinement_flags_adp
 _atom_site_refinement_flags_occupancy
 _atom_site_disorder_assembly
 _atom_site_disorder_group
N1 N 0.0000 0.0000 0.0000 0.038(3) Uani 1 24 d S T P . .
B1 B 0.0000 0.0000 0.2500 0.051(3) Uani 1 8 d S T P . .
F1 F 0.0775(2) 0.0000 0.1941(3) 0.093(3) Uani 1 2 d S T P . .
C2 C 0.1966(5) 0.1966(5) 0.1966(5) 0.075(5) Uani 0.375 3 d DS T P . .
C1 C 0.2500 0.2500 0.1313(7) 0.150(13) Uani 0.5 4 d DS T P . .
N3 N 0.1966(5) 0.1966(5) 0.1966(5) 0.075(5) Uani 0.125 3 d DS T P . .
N2 N 0.2500 0.2500 0.1313(7) 0.150(13) Uani 0.1667 4 d DS T P . .
 
 
_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
B1 F1 1.367(4) 85_445 ?
B1 F1 1.367(4) 2 ?
B1 F1 1.367(4) 86_445 ?
B1 F1 1.367(4) . ?
C2 C1 1.428(6) . ?
C2 N2 1.428(6) 5 ?
C2 C1 1.428(6) 5 ?
C2 N2 1.428(6) 9 ?
C2 C1 1.428(6) 9 ?
C2 C2 1.528(15) 40_544 ?
C2 C2 1.528(15) 63_454 ?
C2 N3 1.528(15) 85_445 ?
C2 N3 1.528(15) 63_454 ?
C2 N3 1.528(15) 40_544 ?
C2 C2 1.528(15) 85_445 ?
C1 N3 1.428(6) 74 ?
C1 C2 1.428(6) 74 ?
C1 N3 1.428(6) 40_544 ?
C1 N3 1.428(6) 63_454 ?
C1 C2 1.428(6) 63_454 ?
C1 C2 1.428(6) 40_544 ?
 
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
F1 B1 F1 110.03(16) 85_445 2 ?
F1 B1 F1 108.4(3) 85_445 86_445 ?
F1 B1 F1 110.03(16) 2 86_445 ?
F1 B1 F1 110.03(16) 85_445 . ?
F1 B1 F1 108.4(3) 2 . ?
F1 B1 F1 110.03(16) 86_445 . ?
C1 C2 N2 114.4 . 5 ?
C1 C2 C1 114.4(5) . 5 ?
N2 C2 C1 0.0 5 5 ?
C1 C2 N2 114.4 . 9 ?
N2 C2 N2 114.4(5) 5 9 ?
C1 C2 N2 114.4(5) 5 9 ?
C1 C2 C1 114.4(5) . 9 ?
N2 C2 C1 114.4 5 9 ?
C1 C2 C1 114.4(5) 5 9 ?
N2 C2 C1 0.0 9 9 ?
C1 C2 C2 57.6(4) . 40_544 ?
N2 C2 C2 130.8(7) 5 40_544 ?
C1 C2 C2 130.8(7) 5 40_544 ?
N2 C2 C2 57.6(4) 9 40_544 ?
C1 C2 C2 57.6(4) 9 40_544 ?
C1 C2 C2 57.6(4) . 63_454 ?
N2 C2 C2 57.6(4) 5 63_454 ?
C1 C2 C2 57.6(4) 5 63_454 ?
N2 C2 C2 130.8(7) 9 63_454 ?
C1 C2 C2 130.8(7) 9 63_454 ?
C2 C2 C2 89.996(2) 40_544 63_454 ?
C1 C2 N3 130.8(7) . 85_445 ?
N2 C2 N3 57.6(4) 5 85_445 ?
C1 C2 N3 57.6(4) 5 85_445 ?
N2 C2 N3 57.6(4) 9 85_445 ?
C1 C2 N3 57.6(4) 9 85_445 ?
C2 C2 N3 89.996(1) 40_544 85_445 ?
C2 C2 N3 89.996(1) 63_454 85_445 ?
C1 C2 N3 57.6(4) . 63_454 ?
N2 C2 N3 57.6(4) 5 63_454 ?
C1 C2 N3 57.6(4) 5 63_454 ?
N2 C2 N3 130.8(7) 9 63_454 ?
C1 C2 N3 130.8(7) 9 63_454 ?
C2 C2 N3 89.996(2) 40_544 63_454 ?
C2 C2 N3 0.0(11) 63_454 63_454 ?
N3 C2 N3 89.996(1) 85_445 63_454 ?
C1 C2 N3 57.6(4) . 40_544 ?
N2 C2 N3 130.8(7) 5 40_544 ?
C1 C2 N3 130.8(7) 5 40_544 ?
N2 C2 N3 57.6(4) 9 40_544 ?
C1 C2 N3 57.6(4) 9 40_544 ?
C2 C2 N3 0.0(11) 40_544 40_544 ?
C2 C2 N3 89.996(2) 63_454 40_544 ?
N3 C2 N3 89.996(1) 85_445 40_544 ?
N3 C2 N3 89.996(2) 63_454 40_544 ?
C1 C2 C2 130.8(7) . 85_445 ?
N2 C2 C2 57.6(4) 5 85_445 ?
C1 C2 C2 57.6(4) 5 85_445 ?
N2 C2 C2 57.6(4) 9 85_445 ?
C1 C2 C2 57.6(4) 9 85_445 ?
C2 C2 C2 89.996(1) 40_544 85_445 ?
C2 C2 C2 89.996(1) 63_454 85_445 ?
N3 C2 C2 0.0 85_445 85_445 ?
N3 C2 C2 90.0 63_454 85_445 ?
N3 C2 C2 90.0 40_544 85_445 ?
N3 C1 C2 0.0 74 74 ?
N3 C1 N3 64.7(8) 74 40_544 ?
C2 C1 N3 64.7(8) 74 40_544 ?
N3 C1 N3 64.7(8) 74 63_454 ?
C2 C1 N3 64.7(8) 74 63_454 ?
N3 C1 N3 98.4(14) 40_544 63_454 ?
N3 C1 C2 64.7 74 63_454 ?
C2 C1 C2 64.7(8) 74 63_454 ?
N3 C1 C2 98.4 40_544 63_454 ?
N3 C1 C2 0.0 63_454 63_454 ?
N3 C1 C2 64.7 74 40_544 ?
C2 C1 C2 64.7(8) 74 40_544 ?
N3 C1 C2 0.0 40_544 40_544 ?
N3 C1 C2 98.4 63_454 40_544 ?
C2 C1 C2 98.4(14) 63_454 40_544 ?
N3 C1 C2 98.4 74 . ?
C2 C1 C2 98.4(14) 74 . ?
N3 C1 C2 64.7 40_544 . ?
N3 C1 C2 64.7 63_454 . ?
C2 C1 C2 64.7(8) 63_454 . ?
C2 C1 C2 64.7(8) 40_544 . ?
 
_refine_diff_density_max    0.534
_refine_diff_density_min   -0.487
_refine_diff_density_rms    0.122



# start Validation Reply Form
_vrf_PLAT084_3
;
PROBLEM: High wR2 Value (i.e. > 0.25) ...................       0.49 Report
RESPONSE: High temperature resulted in poor quality of the crystal
;
# end Validation Reply Form
