# Electronic Supplementary Material (ESI) for Journal of Materials Chemistry C.
# This journal is © The Royal Society of Chemistry 2019

####################################################################### 
# 
# This file contains crystal structure data downloaded from the 
# Cambridge Structural Database (CSD) hosted by the Cambridge 
# Crystallographic Data Centre (CCDC).
# 
# Full information about CCDC data access policies and citation 
# guidelines are available at http://www.ccdc.cam.ac.uk/access/V1 
# 
# Audit and citation data items may have been added by the CCDC. 
# Please retain this information to preserve the provenance of 
# this file and to allow appropriate attribution of the data. 
# 
#######################################################################

data_P21
_database_code_depnum_ccdc_archive 'CCDC 1902122'
loop_
_audit_author_name
_audit_author_address
'Gao Ji-Xing' 'Southeast University'
_audit_update_record             
;
2019-03-09 deposited with the CCDC.	2019-04-10 downloaded from the CCDC.
;

_audit_creation_method           SHELXL-2014/7
_shelx_SHELXL_version_number     2014/7
_chemical_name_systematic        ?
_chemical_name_common            ?
_chemical_melting_point          ?
_chemical_formula_moiety         'C6 H18 N3, B F4, 2(Cl)'
_chemical_formula_sum            'C6 H18 B Cl2 F4 N3'
_chemical_formula_weight         289.94

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'
Cl Cl 0.1484 0.1585 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'

_space_group_crystal_system      monoclinic
_space_group_IT_number           4
_space_group_name_H-M_alt        'P 21'
_space_group_name_Hall           'P 2yb'

_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+1/2, -z'

_cell_length_a                   8.0679(2)
_cell_length_b                   10.5006(3)
_cell_length_c                   14.0399(4)
_cell_angle_alpha                90
_cell_angle_beta                 90.802(2)
_cell_angle_gamma                90
_cell_volume                     1189.31(6)
_cell_formula_units_Z            4
_cell_measurement_temperature    298(2)
_cell_measurement_reflns_used    8218
_cell_measurement_theta_min      2.5810
_cell_measurement_theta_max      31.4180

_exptl_crystal_description       Block
_exptl_crystal_colour            Colourless
_exptl_crystal_density_meas      ?
_exptl_crystal_density_method    ?
_exptl_crystal_density_diffrn    1.619
_exptl_crystal_F_000             600
_exptl_transmission_factor_min   ?
_exptl_transmission_factor_max   ?
_exptl_crystal_size_max          0.270
_exptl_crystal_size_mid          0.260
_exptl_crystal_size_min          0.260
_exptl_absorpt_coefficient_mu    0.574
_shelx_estimated_absorpt_T_min   0.860
_shelx_estimated_absorpt_T_max   0.865
_exptl_absorpt_correction_type   multi-scan
_exptl_absorpt_correction_T_min  0.856
_exptl_absorpt_correction_T_max  0.861
_exptl_absorpt_process_details   'CrysAlisPro 1.171.39.46 (Rigaku OD, 2018)'
_exptl_absorpt_special_details   ?
_diffrn_ambient_temperature      298(2)
_diffrn_radiation_wavelength     0.71073
_diffrn_radiation_type           MoK\a
_diffrn_source                   'Rotating-anode X-ray tube'
_diffrn_measurement_device_type  'XtaLAB Synergy R, DW system, HyPix'
_diffrn_measurement_method       'four-circle diffractometer'
_diffrn_detector_area_resol_mean ?
_diffrn_reflns_number            10402
_diffrn_reflns_av_unetI/netI     0.0279
_diffrn_reflns_av_R_equivalents  0.0194
_diffrn_reflns_limit_h_min       -9
_diffrn_reflns_limit_h_max       10
_diffrn_reflns_limit_k_min       -13
_diffrn_reflns_limit_k_max       13
_diffrn_reflns_limit_l_min       -17
_diffrn_reflns_limit_l_max       15
_diffrn_reflns_theta_min         2.422
_diffrn_reflns_theta_max         26.994
_diffrn_reflns_theta_full        25.242
_diffrn_measured_fraction_theta_max 0.998
_diffrn_measured_fraction_theta_full 0.998
_diffrn_reflns_Laue_measured_fraction_max 0.998
_diffrn_reflns_Laue_measured_fraction_full 0.998
_diffrn_reflns_point_group_measured_fraction_max 0.934
_diffrn_reflns_point_group_measured_fraction_full 0.942
_reflns_number_total             5208
_reflns_number_gt                4517
_reflns_threshold_expression     'I > 2σ(I)'
_reflns_Friedel_coverage         0.773
_reflns_Friedel_fraction_max     0.863
_reflns_Friedel_fraction_full    0.878

_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       'CrysAlisPro 1.171.39.46 (Rigaku OD, 2018)'
_computing_cell_refinement       'CrysAlisPro 1.171.39.46 (Rigaku OD, 2018)'
_computing_data_reduction        'CrysAlisPro 1.171.39.46 (Rigaku OD, 2018)'
_computing_structure_solution    'SHELXL-2014/7 (Sheldrick, 2014)'
_computing_structure_refinement  'SHELXL-2014/7 (Sheldrick, 2014)'
_computing_molecular_graphics    'DIAMOND (Brandenburg & Putz, 2005)'
_computing_publication_material  'SHELXL-2014/7 (Sheldrick, 2014)'
_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)+(0.0412P)²+0.4699P] where P=(Fo²+2Fc²)/3'
_atom_sites_solution_primary     ?
_atom_sites_solution_secondary   ?
_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 x determined using 1832 quotients [(I+)-(I-)]/[(I+)+(I-)]
 (Parsons, Flack and Wagner, Acta Cryst. B69 (2013) 249-259).
;
_refine_ls_abs_structure_Flack   0.06(2)
_chemical_absolute_configuration ?
_refine_ls_number_reflns         5208
_refine_ls_number_parameters     289
_refine_ls_number_restraints     1
_refine_ls_R_factor_all          0.0354
_refine_ls_R_factor_gt           0.0324
_refine_ls_wR_factor_ref         0.0814
_refine_ls_wR_factor_gt          0.0800
_refine_ls_goodness_of_fit_ref   1.000
_refine_ls_restrained_S_all      1.000
_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
Cl1 Cl 0.00897(9) 0.04632(7) 0.17712(6) 0.02787(18) Uani 1 1 d . . . . .
Cl2 Cl 0.98558(11) 0.39015(8) 0.15575(6) 0.0332(2) Uani 1 1 d . . . . .
Cl3 Cl 0.49681(10) 0.53438(7) 0.33813(6) 0.0327(2) Uani 1 1 d . . . . .
Cl4 Cl 0.49855(9) 0.88830(7) 0.32546(5) 0.02681(18) Uani 1 1 d . . . . .
B1 B 0.9719(5) 0.4787(4) 0.4767(3) 0.0277(8) Uani 1 1 d . . . . .
B2 B 0.4883(5) 0.9494(4) 0.0254(3) 0.0275(8) Uani 1 1 d . . . . .
F1 F 0.9640(3) 0.6116(2) 0.4777(2) 0.0557(7) Uani 1 1 d . . . . .
F2 F 1.0843(3) 0.4449(3) 0.54655(18) 0.0534(6) Uani 1 1 d . . . . .
F3 F 0.8190(3) 0.4300(3) 0.4970(2) 0.0703(9) Uani 1 1 d . . . . .
F4 F 1.0284(4) 0.4382(3) 0.3894(2) 0.0744(9) Uani 1 1 d . . . . .
F5 F 0.5990(3) 0.9928(3) 0.09311(19) 0.0620(7) Uani 1 1 d . . . . .
F6 F 0.4797(3) 0.8170(2) 0.02836(19) 0.0508(7) Uani 1 1 d . . . . .
F7 F 0.5440(3) 0.9815(2) -0.06455(17) 0.0508(6) Uani 1 1 d . . . . .
F8 F 0.3323(3) 0.9988(3) 0.0378(2) 0.0659(8) Uani 1 1 d . . . . .
C1 C 0.3518(4) 0.2513(3) 0.4554(2) 0.0272(7) Uani 1 1 d . . . . .
H1C H 0.2886 0.3278 0.4684 0.033 Uiso 1 1 calc R U . . .
H1D H 0.3289 0.1908 0.5057 0.033 Uiso 1 1 calc R U . . .
C2 C 0.2902(4) 0.1959(3) 0.3624(2) 0.0264(7) Uani 1 1 d . . . . .
H2C H 0.3551 0.1206 0.3484 0.032 Uiso 1 1 calc R U . . .
H2D H 0.1762 0.1691 0.3701 0.032 Uiso 1 1 calc R U . . .
C3 C 0.3904(4) 0.2336(3) 0.1953(2) 0.0261(7) Uani 1 1 d . . . . .
H3C H 0.3509 0.2771 0.1384 0.031 Uiso 1 1 calc R U . . .
H3D H 0.3638 0.1441 0.1880 0.031 Uiso 1 1 calc R U . . .
C4 C 0.5770(4) 0.2473(3) 0.2012(2) 0.0254(7) Uani 1 1 d . . . . .
H4A H 0.6024 0.3303 0.2278 0.031 Uiso 1 1 calc R U . . .
H4B H 0.6193 0.2460 0.1368 0.031 Uiso 1 1 calc R U . . .
C5 C 0.7509(4) 0.1912(3) 0.3503(2) 0.0259(7) Uani 1 1 d . . . . .
H5A H 0.7810 0.2800 0.3432 0.031 Uiso 1 1 calc R U . . .
H5B H 0.8529 0.1435 0.3589 0.031 Uiso 1 1 calc R U . . .
C6 C 0.6515(4) 0.1783(3) 0.4402(2) 0.0236(7) Uani 1 1 d . . . . .
H6A H 0.5901 0.0990 0.4369 0.028 Uiso 1 1 calc R U . . .
H6B H 0.7283 0.1719 0.4938 0.028 Uiso 1 1 calc R U . . .
C7 C 0.8454(4) 0.7310(3) 0.0745(2) 0.0257(7) Uani 1 1 d . . . . .
H7A H 0.8985 0.8067 0.1002 0.031 Uiso 1 1 calc R U . . .
H7B H 0.7746 0.7574 0.0217 0.031 Uiso 1 1 calc R U . . .
C8 C 0.7391(4) 0.6735(3) 0.1502(2) 0.0284(7) Uani 1 1 d . . . . .
H8A H 0.6496 0.7323 0.1636 0.034 Uiso 1 1 calc R U . . .
H8B H 0.6895 0.5961 0.1250 0.034 Uiso 1 1 calc R U . . .
C9 C 0.9060(4) 0.7535(3) 0.2919(2) 0.0228(6) Uani 1 1 d . . . . .
H9A H 0.8596 0.7604 0.3550 0.027 Uiso 1 1 calc R U . . .
H9B H 0.8764 0.8305 0.2574 0.027 Uiso 1 1 calc R U . . .
C10 C 1.0928(4) 0.7481(3) 0.3018(2) 0.0259(7) Uani 1 1 d . . . . .
H10A H 1.1262 0.8043 0.3535 0.031 Uiso 1 1 calc R U . . .
H10B H 1.1238 0.6623 0.3203 0.031 Uiso 1 1 calc R U . . .
C11 C 1.2257(4) 0.6779(3) 0.1466(2) 0.0241(6) Uani 1 1 d . . . . .
H11A H 1.1866 0.5988 0.1740 0.029 Uiso 1 1 calc R U . . .
H11B H 1.3451 0.6709 0.1409 0.029 Uiso 1 1 calc R U . . .
C12 C 1.1514(4) 0.6901(3) 0.0473(2) 0.0264(7) Uani 1 1 d . . . . .
H12A H 1.1543 0.7790 0.0286 0.032 Uiso 1 1 calc R U . . .
H12B H 1.2202 0.6431 0.0034 0.032 Uiso 1 1 calc R U . . .
N1 N 0.5315(3) 0.2840(3) 0.46010(19) 0.0230(5) Uani 1 1 d . . . . .
H1A H 0.5542 0.3145 0.5180 0.028 Uiso 1 1 calc R U . . .
H1B H 0.5498 0.3465 0.4187 0.028 Uiso 1 1 calc R U . . .
N2 N 0.2981(3) 0.2845(3) 0.27888(19) 0.0232(5) Uani 1 1 d . . . . .
H2A H 0.1951 0.3031 0.2601 0.028 Uiso 1 1 calc R U . . .
H2B H 0.3461 0.3567 0.2978 0.028 Uiso 1 1 calc R U . . .
N3 N 0.6703(3) 0.1481(2) 0.25895(18) 0.0208(5) Uani 1 1 d . . . . .
H3A H 0.6001 0.0856 0.2725 0.025 Uiso 1 1 calc R U . . .
H3B H 0.7486 0.1152 0.2223 0.025 Uiso 1 1 calc R U . . .
N4 N 0.9772(3) 0.6432(3) 0.03724(19) 0.0239(6) Uani 1 1 d . . . . .
H4C H 0.9695 0.5690 0.0676 0.029 Uiso 1 1 calc R U . . .
H4D H 0.9560 0.6286 -0.0242 0.029 Uiso 1 1 calc R U . . .
N5 N 0.8260(3) 0.6420(3) 0.24194(19) 0.0236(5) Uani 1 1 d . . . . .
H5C H 0.9037 0.5841 0.2304 0.028 Uiso 1 1 calc R U . . .
H5D H 0.7532 0.6068 0.2811 0.028 Uiso 1 1 calc R U . . .
N6 N 1.1896(3) 0.7837(2) 0.21527(18) 0.0207(5) Uani 1 1 d . . . . .
H6C H 1.2856 0.8173 0.2346 0.025 Uiso 1 1 calc R U . . .
H6D H 1.1339 0.8442 0.1840 0.025 Uiso 1 1 calc R U . . .


_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 F3 1.370(5) . ?
B1 F2 1.372(4) . ?
B1 F4 1.381(5) . ?
B1 F1 1.397(4) . ?
B2 F5 1.373(4) . ?
B2 F8 1.374(5) . ?
B2 F7 1.388(5) . ?
B2 F6 1.393(4) . ?
C1 N1 1.491(4) . ?
C1 C2 1.507(5) . ?
C2 N2 1.499(4) . ?
C3 N2 1.497(4) . ?
C3 C4 1.513(4) . ?
C4 N3 1.514(4) . ?
C5 N3 1.499(4) . ?
C5 C6 1.511(5) . ?
C6 N1 1.502(4) . ?
C7 C8 1.502(5) . ?
C7 N4 1.507(4) . ?
C8 N5 1.495(4) . ?
C9 N5 1.506(4) . ?
C9 C10 1.513(4) . ?
C10 N6 1.501(4) . ?
C11 N6 1.502(4) . ?
C11 C12 1.516(4) . ?
C12 N4 1.494(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
F3 B1 F2 110.0(3) . . ?
F3 B1 F4 112.3(3) . . ?
F2 B1 F4 109.3(3) . . ?
F3 B1 F1 109.3(3) . . ?
F2 B1 F1 106.4(3) . . ?
F4 B1 F1 109.4(3) . . ?
F5 B2 F8 112.0(3) . . ?
F5 B2 F7 109.5(3) . . ?
F8 B2 F7 109.5(3) . . ?
F5 B2 F6 110.0(3) . . ?
F8 B2 F6 109.1(3) . . ?
F7 B2 F6 106.7(3) . . ?
N1 C1 C2 115.8(3) . . ?
N2 C2 C1 114.9(3) . . ?
N2 C3 C4 115.4(3) . . ?
C3 C4 N3 116.8(3) . . ?
N3 C5 C6 117.3(3) . . ?
N1 C6 C5 116.1(3) . . ?
C8 C7 N4 114.4(3) . . ?
N5 C8 C7 115.7(2) . . ?
N5 C9 C10 115.7(2) . . ?
N6 C10 C9 116.4(3) . . ?
N6 C11 C12 116.7(2) . . ?
N4 C12 C11 114.7(3) . . ?
C1 N1 C6 116.8(3) . . ?
C3 N2 C2 114.8(2) . . ?
C5 N3 C4 117.2(2) . . ?
C12 N4 C7 115.7(2) . . ?
C8 N5 C9 115.0(2) . . ?
C10 N6 C11 116.3(2) . . ?

loop_
_geom_torsion_atom_site_label_1
_geom_torsion_atom_site_label_2
_geom_torsion_atom_site_label_3
_geom_torsion_atom_site_label_4
_geom_torsion
_geom_torsion_site_symmetry_1
_geom_torsion_site_symmetry_2
_geom_torsion_site_symmetry_3
_geom_torsion_site_symmetry_4
_geom_torsion_publ_flag
N1 C1 C2 N2 -65.1(4) . . . . ?
N2 C3 C4 N3 81.5(3) . . . . ?
N3 C5 C6 N1 -83.3(3) . . . . ?
N4 C7 C8 N5 65.6(4) . . . . ?
N5 C9 C10 N6 79.1(3) . . . . ?
N6 C11 C12 N4 -84.7(3) . . . . ?
C2 C1 N1 C6 -57.0(4) . . . . ?
C5 C6 N1 C1 113.0(3) . . . . ?
C4 C3 N2 C2 -82.3(3) . . . . ?
C1 C2 N2 C3 125.5(3) . . . . ?
C6 C5 N3 C4 92.4(3) . . . . ?
C3 C4 N3 C5 -111.3(3) . . . . ?
C11 C12 N4 C7 77.5(3) . . . . ?
C8 C7 N4 C12 -121.8(3) . . . . ?
C7 C8 N5 C9 59.8(4) . . . . ?
C10 C9 N5 C8 -116.1(3) . . . . ?
C9 C10 N6 C11 -88.1(3) . . . . ?
C12 C11 N6 C10 116.9(3) . . . . ?

loop_
_geom_hbond_atom_site_label_D
_geom_hbond_atom_site_label_H
_geom_hbond_atom_site_label_A
_geom_hbond_distance_DH
_geom_hbond_distance_HA
_geom_hbond_distance_DA
_geom_hbond_angle_DHA
_geom_hbond_site_symmetry_A
C1 H1C F2 0.97 2.34 3.242(4) 153.9 1_455
C1 H1C F4 0.97 2.63 3.384(5) 134.8 1_455
C1 H1D F1 0.97 2.52 3.098(4) 118.2 2_646
C2 H2C Cl4 0.97 2.72 3.681(3) 170.5 1_545
C2 H2D F1 0.97 2.51 3.188(4) 127.2 2_646
C3 H3C F7 0.97 2.53 3.233(4) 128.8 2_645
C3 H3D F8 0.97 2.61 3.341(4) 132.0 1_545
C4 H4A Cl3 0.97 2.78 3.639(3) 147.4 .
C4 H4B F6 0.97 2.55 3.330(4) 137.0 2_645
C5 H5B F2 0.97 2.52 3.240(4) 131.1 2_746
C6 H6A Cl4 0.97 2.80 3.651(3) 146.6 1_545
C6 H6B F1 0.97 2.59 3.367(4) 137.6 2_746
C7 H7A Cl1 0.97 2.88 3.838(3) 171.8 1_665
C7 H7B F6 0.97 2.46 3.144(4) 127.0 .
C8 H8A F6 0.97 2.49 3.078(4) 118.9 .
C8 H8B F7 0.97 2.38 3.263(4) 150.8 2_645
C8 H8B F8 0.97 2.51 3.259(4) 134.2 2_645
C9 H9A F1 0.97 2.46 3.035(4) 117.3 .
C9 H9A F2 0.97 2.42 3.031(4) 120.7 2_756
C9 H9B Cl1 0.97 2.75 3.574(3) 142.7 1_665
C10 H10A F3 0.97 2.51 3.475(4) 170.9 2_756
C11 H11A Cl2 0.97 2.74 3.592(3) 147.6 .
C11 H11B F6 0.97 2.47 3.031(4) 116.9 1_655
C11 H11B F7 0.97 2.44 3.015(4) 118.0 2_745
C12 H12B F5 0.97 2.55 3.513(5) 171.3 2_745
N1 H1A Cl4 0.89 2.37 3.216(3) 157.7 2_646
N1 H1B Cl3 0.89 2.31 3.148(3) 156.6 .
N2 H2A Cl2 0.89 2.40 3.234(3) 155.6 1_455
N2 H2B Cl3 0.89 2.29 3.179(3) 173.4 .
N3 H3A Cl4 0.89 2.35 3.205(3) 160.6 1_545
N3 H3B Cl1 0.89 2.32 3.165(3) 158.8 1_655
N4 H4C Cl2 0.89 2.25 3.135(3) 171.4 .
N4 H4D Cl1 0.89 2.34 3.180(3) 158.5 2_655
N5 H5C Cl2 0.89 2.39 3.187(3) 149.6 .
N5 H5D Cl3 0.89 2.35 3.202(3) 159.1 .
N6 H6C Cl4 0.89 2.25 3.116(2) 163.2 1_655
N6 H6D Cl1 0.89 2.35 3.161(3) 151.3 1_665

_refine_diff_density_max         0.359
_refine_diff_density_min         -0.277
_refine_diff_density_rms         0.052

####################################################################### 
# 
# This file contains crystal structure data downloaded from the 
# Cambridge Structural Database (CSD) hosted by the Cambridge 
# Crystallographic Data Centre (CCDC).
# 
# Full information about CCDC data access policies and citation 
# guidelines are available at http://www.ccdc.cam.ac.uk/access/V1 
# 
# Audit and citation data items may have been added by the CCDC. 
# Please retain this information to preserve the provenance of 
# this file and to allow appropriate attribution of the data. 
# 
#######################################################################

data_P63mmc
_database_code_depnum_ccdc_archive 'CCDC 1902123'
loop_
_audit_author_name
_audit_author_address
'Gao Ji-Xing' 'Southeast University'
_audit_update_record             
;
2019-03-09 deposited with the CCDC.	2019-04-10 downloaded from the CCDC.
;

_audit_creation_method           SHELXL-2014/7
_shelx_SHELXL_version_number     2014/7
_chemical_name_systematic        ?
_chemical_name_common            ?
_chemical_melting_point          ?
_chemical_formula_moiety         'B F4, 3(C2 H6 N), 2(Cl)'
_chemical_formula_sum            'C6 H18 B Cl2 F4 N3'
_chemical_formula_weight         289.94

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'
Cl Cl 0.1484 0.1585 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'

_space_group_crystal_system      hexagonal
_space_group_IT_number           194
_space_group_name_H-M_alt        'P 63/m m c'
_space_group_name_Hall           '-P 6c 2c'

_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'
'-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                   8.1276(7)
_cell_length_b                   8.1276(7)
_cell_length_c                   10.5327(13)
_cell_angle_alpha                90
_cell_angle_beta                 90
_cell_angle_gamma                120
_cell_volume                     602.55(13)
_cell_formula_units_Z            2
_cell_measurement_temperature    413(2)
_cell_measurement_reflns_used    1742
_cell_measurement_theta_min      2.8590
_cell_measurement_theta_max      28.9430

_exptl_crystal_description       Block
_exptl_crystal_colour            Colourless
_exptl_crystal_density_meas      ?
_exptl_crystal_density_method    ?
_exptl_crystal_density_diffrn    1.598
_exptl_crystal_F_000             300
_exptl_transmission_factor_min   ?
_exptl_transmission_factor_max   ?
_exptl_crystal_size_max          0.270
_exptl_crystal_size_mid          0.260
_exptl_crystal_size_min          0.260
_exptl_absorpt_coefficient_mu    0.567
_shelx_estimated_absorpt_T_min   0.862
_shelx_estimated_absorpt_T_max   0.867
_exptl_absorpt_correction_type   multi-scan
_exptl_absorpt_correction_T_min  0.858
_exptl_absorpt_correction_T_max  0.863
_exptl_absorpt_process_details   'CrysAlisPro 1.171.39.46 (Rigaku OD, 2018)'
_exptl_absorpt_special_details   ?
_diffrn_ambient_temperature      413(2)
_diffrn_radiation_wavelength     0.71073
_diffrn_radiation_type           MoK\a
_diffrn_source                   'Rotating-anode X-ray tube'
_diffrn_measurement_device_type  'XtaLAB Synergy R, DW system, HyPix'
_diffrn_measurement_method       'four-circle diffractometer'
_diffrn_detector_area_resol_mean ?
_diffrn_reflns_number            2370
_diffrn_reflns_av_unetI/netI     0.0216
_diffrn_reflns_av_R_equivalents  0.0381
_diffrn_reflns_limit_h_min       -10
_diffrn_reflns_limit_h_max       10
_diffrn_reflns_limit_k_min       -7
_diffrn_reflns_limit_k_max       10
_diffrn_reflns_limit_l_min       -13
_diffrn_reflns_limit_l_max       11
_diffrn_reflns_theta_min         2.894
_diffrn_reflns_theta_max         26.987
_diffrn_reflns_theta_full        25.242
_diffrn_measured_fraction_theta_max 0.993
_diffrn_measured_fraction_theta_full 0.992
_diffrn_reflns_Laue_measured_fraction_max 0.993
_diffrn_reflns_Laue_measured_fraction_full 0.992
_diffrn_reflns_point_group_measured_fraction_max 0.993
_diffrn_reflns_point_group_measured_fraction_full 0.992
_reflns_number_total             286
_reflns_number_gt                239
_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       'CrysAlisPro 1.171.39.46 (Rigaku OD, 2018)'
_computing_cell_refinement       'CrysAlisPro 1.171.39.46 (Rigaku OD, 2018)'
_computing_data_reduction        'CrysAlisPro 1.171.39.46 (Rigaku OD, 2018)'
_computing_structure_solution    'SHELXL-2014/7 (Sheldrick, 2014)'
_computing_structure_refinement  'SHELXL-2014/7 (Sheldrick, 2014)'
_computing_molecular_graphics    'DIAMOND (Brandenburg & Putz, 2005)'
_computing_publication_material  'SHELXL-2014/7 (Sheldrick, 2014)'
_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)+(0.2000P)²] where P=(Fo²+2Fc²)/3'
_atom_sites_solution_primary     ?
_atom_sites_solution_secondary   ?
_atom_sites_solution_hydrogens   difmap
_refine_ls_hydrogen_treatment    refU
_refine_ls_extinction_method     none
_refine_ls_extinction_coef       .
_refine_ls_number_reflns         286
_refine_ls_number_parameters     34
_refine_ls_number_restraints     30
_refine_ls_R_factor_all          0.1203
_refine_ls_R_factor_gt           0.1161
_refine_ls_wR_factor_ref         0.3973
_refine_ls_wR_factor_gt          0.3897
_refine_ls_goodness_of_fit_ref   1.959
_refine_ls_restrained_S_all      1.938
_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
Cl1 Cl 0.6667 0.3333 0.07256(17) 0.0622(16) Uani 1 6 d S T P . .
B1 B 1.0000 1.0000 0.0000 0.133(8) Uani 1 12 d DS TU P . .
F1 F 1.0000 1.0000 0.1292(15) 0.171(6) Uani 1 6 d DS TU P . .
F2 F 0.9026(10) 0.805(2) 0.020(2) 0.143(6) Uani 0.3333 2 d DS TU P . .
C1 C 0.2931(11) 0.4047(11) 0.260(3) 0.109(7) Uani 0.5 1 d D . P . .
H1A H 0.3207 0.4521 0.3453 0.3(3) Uiso 0.5 1 d R . P . .
H1B H 0.2767 0.2792 0.2500 0.072(18) Uiso 1 2 d R . P . .
N1 N 0.4558(6) 0.5442(6) 0.1820(9) 0.064(3) Uani 0.5 2 d DS T P . .
H1C H 0.4110 0.5890 0.1210 0.11(6) Uiso 0.5 2 d R . P . .
H1D H 0.5137 0.4863 0.1457 0.4(6) Uiso 0.5 2 d R . 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 1.361(16) . ?
B1 F1 1.361(16) 13_775 ?
B1 F2 1.386(13) 14_565 ?
B1 F2 1.386(13) 2_765 ?
B1 F2 1.386(13) 13_775 ?
B1 F2 1.387(13) . ?
B1 F2 1.387(13) 15_655 ?
B1 F2 1.387(13) 3_675 ?
F2 F2 1.433(16) 14_565 ?
F2 F2 1.433(16) 15_655 ?
C1 C1 0.21(6) 16_556 ?
C1 N1 1.382(17) 16_556 ?
C1 C1 1.476(17) 20 ?
C1 N1 1.486(18) . ?
C1 C1 1.491(17) 11 ?
N1 C1 1.382(17) 10_665 ?
N1 C1 1.382(17) 16_556 ?
N1 N1 1.433(19) 16_556 ?
N1 C1 1.486(18) 19_665 ?

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 180.0 . 13_775 ?
F1 B1 F2 98.6(9) . 14_565 ?
F1 B1 F2 81.4(9) 13_775 14_565 ?
F1 B1 F2 81.4(9) . 2_765 ?
F1 B1 F2 98.6(9) 13_775 2_765 ?
F2 B1 F2 180.0(7) 14_565 2_765 ?
F1 B1 F2 98.6(9) . 13_775 ?
F1 B1 F2 81.4(9) 13_775 13_775 ?
F2 B1 F2 117.8(5) 14_565 13_775 ?
F2 B1 F2 62.2(5) 2_765 13_775 ?
F1 B1 F2 81.4(9) . . ?
F1 B1 F2 98.6(9) 13_775 . ?
F2 B1 F2 62.2(5) 14_565 . ?
F2 B1 F2 117.8(5) 2_765 . ?
F2 B1 F2 180.0 13_775 . ?
F1 B1 F2 98.6(9) . 15_655 ?
F1 B1 F2 81.4(9) 13_775 15_655 ?
F2 B1 F2 117.8(5) 14_565 15_655 ?
F2 B1 F2 62.2(5) 2_765 15_655 ?
F2 B1 F2 117.8(5) 13_775 15_655 ?
F2 B1 F2 62.2(5) . 15_655 ?
F1 B1 F2 81.4(9) . 3_675 ?
F1 B1 F2 98.6(9) 13_775 3_675 ?
F2 B1 F2 62.2(5) 14_565 3_675 ?
F2 B1 F2 117.8(5) 2_765 3_675 ?
F2 B1 F2 62.2(5) 13_775 3_675 ?
F2 B1 F2 117.8(5) . 3_675 ?
F2 B1 F2 180.0 15_655 3_675 ?
B1 F2 F2 58.9(2) . 14_565 ?
B1 F2 F2 58.9(2) . 15_655 ?
F2 F2 F2 111.9(15) 14_565 15_655 ?
C1 C1 N1 116.3(13) 16_556 16_556 ?
C1 C1 C1 90.007(8) 16_556 20 ?
N1 C1 C1 123.1(7) 16_556 20 ?
C1 C1 N1 56.5(10) 16_556 . ?
N1 C1 N1 59.8(8) 16_556 . ?
C1 C1 N1 120.5(5) 20 . ?
C1 C1 C1 82(2) 16_556 11 ?
N1 C1 C1 127.1(16) 16_556 11 ?
C1 C1 C1 8(2) 20 11 ?
N1 C1 C1 115(2) . 11 ?
C1 N1 C1 125(2) 10_665 16_556 ?
C1 N1 N1 63.7(13) 10_665 16_556 ?
C1 N1 N1 63.7(13) 16_556 16_556 ?
C1 N1 C1 7(2) 10_665 19_665 ?
C1 N1 C1 118.5(7) 16_556 19_665 ?
N1 N1 C1 56.5(10) 16_556 19_665 ?
C1 N1 C1 118.5(7) 10_665 . ?
C1 N1 C1 7(2) 16_556 . ?
N1 N1 C1 56.5(10) 16_556 . ?
C1 N1 C1 111(2) 19_665 . ?

loop_
_geom_torsion_atom_site_label_1
_geom_torsion_atom_site_label_2
_geom_torsion_atom_site_label_3
_geom_torsion_atom_site_label_4
_geom_torsion
_geom_torsion_site_symmetry_1
_geom_torsion_site_symmetry_2
_geom_torsion_site_symmetry_3
_geom_torsion_site_symmetry_4
_geom_torsion_publ_flag
F1 B1 F2 F2 104.6(15) . . . 14_565 ?
F1 B1 F2 F2 -75.4(15) 13_775 . . 14_565 ?
F2 B1 F2 F2 180.000(0) 2_765 . . 14_565 ?
F2 B1 F2 F2 -151(3) 15_655 . . 14_565 ?
F2 B1 F2 F2 29(3) 3_675 . . 14_565 ?
F1 B1 F2 F2 -104.6(15) . . . 15_655 ?
F1 B1 F2 F2 75.4(15) 13_775 . . 15_655 ?
F2 B1 F2 F2 151(3) 14_565 . . 15_655 ?
F2 B1 F2 F2 -29(3) 2_765 . . 15_655 ?
F2 B1 F2 F2 180.000(2) 3_675 . . 15_655 ?
C1 C1 N1 C1 164.6(13) 16_556 . . 10_665 ?
N1 C1 N1 C1 -15.4(13) 16_556 . . 10_665 ?
C1 C1 N1 C1 97.6(9) 20 . . 10_665 ?
C1 C1 N1 C1 104(2) 11 . . 10_665 ?
N1 C1 N1 C1 179.993(7) 16_556 . . 16_556 ?
C1 C1 N1 C1 -67.0(8) 20 . . 16_556 ?
C1 C1 N1 C1 -60(3) 11 . . 16_556 ?
C1 C1 N1 N1 -179.993(6) 16_556 . . 16_556 ?
C1 C1 N1 N1 113.0(8) 20 . . 16_556 ?
C1 C1 N1 N1 120(3) 11 . . 16_556 ?
C1 C1 N1 C1 166.5(10) 16_556 . . 19_665 ?
N1 C1 N1 C1 -13.5(10) 16_556 . . 19_665 ?
C1 C1 N1 C1 99.5(10) 20 . . 19_665 ?
C1 C1 N1 C1 106(3) 11 . . 19_665 ?

_refine_diff_density_max         0.602
_refine_diff_density_min         -0.983
_refine_diff_density_rms         0.146

# start Validation Reply Form

_vrf_PLAT084_P63mmc              
;
PROBLEM: High wR2 Value (i.e. > 0.25) ...................       0.40 Report   
RESPONSE: The quality of crystal is effected by high temperature. 
          Besides, the crystal diffraction point is very poor at 413 K.
;

# end Validation Reply Form


