# Electronic Supplementary Material (ESI) for RSC Advances.
# This journal is © The Royal Society of Chemistry 2022

####################################################################### 
# 
# 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_C6CuCl4_300K
_database_code_depnum_ccdc_archive 'CCDC 2170927'
loop_
_audit_author_name
_audit_author_address
'Huiyeong Ju'
;Korea Basic Science Institute
South Korea
;
_audit_update_record             
;
2022-05-05 deposited with the CCDC.	2022-07-11 downloaded from the CCDC.
;

_audit_creation_method           SHELXL-2018/3
_shelx_SHELXL_version_number     2018/3
_chemical_name_systematic        ?
_chemical_name_common            ?
_chemical_melting_point          ?
_chemical_formula_moiety         'C6 H18 N2, Cl4 Cu'
_chemical_formula_sum            'C6 H18 Cl4 Cu N2'
_chemical_formula_weight         323.56

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'
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'
N N 0.0061 0.0033 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'

_space_group_crystal_system      monoclinic
_space_group_IT_number           14
_space_group_name_H-M_alt        'P 21/n'
_space_group_name_Hall           '-P 2yn'

_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+1/2, y+1/2, -z+1/2'
'-x, -y, -z'
'x-1/2, -y-1/2, z-1/2'

_cell_length_a                   7.2224(6)
_cell_length_b                   7.6112(6)
_cell_length_c                   23.3315(18)
_cell_angle_alpha                90
_cell_angle_beta                 91.930(2)
_cell_angle_gamma                90
_cell_volume                     1281.83(18)
_cell_formula_units_Z            4
_cell_measurement_temperature    300(2)
_cell_measurement_reflns_used    5814
_cell_measurement_theta_min      3.49
_cell_measurement_theta_max      28.23

_exptl_crystal_description       BLOCK
_exptl_crystal_colour            yellow
_exptl_crystal_density_meas      ?
_exptl_crystal_density_method    ?
_exptl_crystal_density_diffrn    1.677
_exptl_crystal_F_000             660
_exptl_transmission_factor_min   ?
_exptl_transmission_factor_max   ?
_exptl_crystal_size_max          0.130
_exptl_crystal_size_mid          0.080
_exptl_crystal_size_min          0.056
_exptl_absorpt_coefficient_mu    2.500
_shelx_estimated_absorpt_T_min   0.737
_shelx_estimated_absorpt_T_max   0.873
_exptl_absorpt_correction_type   multi-scan
_exptl_absorpt_correction_T_min  0.6304
_exptl_absorpt_correction_T_max  0.7457
_exptl_absorpt_process_details   SADABS
_exptl_absorpt_special_details   ?
_diffrn_ambient_temperature      300(2)
_diffrn_radiation_wavelength     0.71073
_diffrn_radiation_type           MoK\a
_diffrn_source                   ?
_diffrn_measurement_device_type  'Bruker APEX-II CCD'
_diffrn_measurement_method       'φ and ω scans'
_diffrn_detector_area_resol_mean ?
_diffrn_reflns_number            22737
_diffrn_reflns_av_unetI/netI     0.0356
_diffrn_reflns_av_R_equivalents  0.0568
_diffrn_reflns_limit_h_min       -9
_diffrn_reflns_limit_h_max       8
_diffrn_reflns_limit_k_min       -10
_diffrn_reflns_limit_k_max       10
_diffrn_reflns_limit_l_min       -31
_diffrn_reflns_limit_l_max       31
_diffrn_reflns_theta_min         2.815
_diffrn_reflns_theta_max         28.286
_diffrn_reflns_theta_full        25.242
_diffrn_measured_fraction_theta_max 0.999
_diffrn_measured_fraction_theta_full 0.999
_diffrn_reflns_Laue_measured_fraction_max 0.999
_diffrn_reflns_Laue_measured_fraction_full 0.999
_diffrn_reflns_point_group_measured_fraction_max 0.999
_diffrn_reflns_point_group_measured_fraction_full 0.999
_reflns_number_total             3182
_reflns_number_gt                2246
_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       'Bruker APEX2'
_computing_cell_refinement       'Bruker SAINT'
_computing_data_reduction        'Bruker SAINT'
_computing_structure_solution    'SHELXT 2014/5 (Sheldrick, 2014)'
_computing_structure_refinement  'SHELXL-2018/3 (Sheldrick, 2018)'
_computing_molecular_graphics    'Bruker SHELXTL'
_computing_publication_material  'Bruker SHELXTL'
_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)+(0.0542P)²+4.0137P] 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_number_reflns         3182
_refine_ls_number_parameters     118
_refine_ls_number_restraints     0
_refine_ls_R_factor_all          0.0793
_refine_ls_R_factor_gt           0.0510
_refine_ls_wR_factor_ref         0.1407
_refine_ls_wR_factor_gt          0.1214
_refine_ls_goodness_of_fit_ref   1.071
_refine_ls_restrained_S_all      1.071
_refine_ls_shift/su_max          0.001
_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
Cu1 Cu 0.49925(7) 0.31907(7) 0.25111(2) 0.02713(17) Uani 1 1 d . . . . .
Cl1 Cl 0.72169(15) 0.52831(14) 0.23785(5) 0.0330(3) Uani 1 1 d . . . . .
Cl2 Cl 0.52571(17) 0.36405(16) 0.34893(5) 0.0377(3) Uani 1 1 d . . . . .
Cl3 Cl 0.27628(15) 0.11058(14) 0.26433(5) 0.0328(3) Uani 1 1 d . . . . .
Cl4 Cl 0.47126(17) 0.27418(15) 0.15359(5) 0.0363(3) Uani 1 1 d . . . . .
N1 N 0.5021(6) 0.7897(5) 0.33779(16) 0.0359(9) Uani 1 1 d . . . . .
H1NA H 0.549557 0.845484 0.308160 0.054 Uiso 1 1 calc R U . . .
H1NB H 0.548406 0.681437 0.340027 0.054 Uiso 1 1 calc R U . . .
H1NC H 0.379434 0.784009 0.332993 0.054 Uiso 1 1 calc R U . . .
N2 N 0.0029(6) 0.3470(5) 0.34267(17) 0.0383(9) Uani 1 1 d . . . . .
H2NA H 0.056948 0.299718 0.312629 0.057 Uiso 1 1 calc R U . . .
H2NB H -0.119074 0.351325 0.335918 0.057 Uiso 1 1 calc R U . . .
H2NC H 0.046128 0.455308 0.348473 0.057 Uiso 1 1 calc R U . . .
C1 C 0.5504(10) 0.8872(9) 0.3919(2) 0.0606(16) Uani 1 1 d . . . . .
H1A H 0.684193 0.895257 0.396124 0.073 Uiso 1 1 calc R U . . .
H1AB H 0.502118 1.005784 0.388544 0.073 Uiso 1 1 calc R U . . .
C2 C 0.4795(12) 0.8071(10) 0.4428(3) 0.0705(19) Uani 1 1 d . . . . .
H2A H 0.523458 0.686904 0.445780 0.085 Uiso 1 1 calc R U . . .
H2AB H 0.345250 0.804460 0.439907 0.085 Uiso 1 1 calc R U . . .
C3 C 0.5419(11) 0.9092(9) 0.4969(3) 0.0697(19) Uani 1 1 d . . . . .
H3A H 0.511431 0.840068 0.530160 0.084 Uiso 1 1 calc R U . . .
H3AB H 0.675602 0.921099 0.497027 0.084 Uiso 1 1 calc R U . . .
C4 C 0.0438(8) 0.2383(7) 0.3943(2) 0.0475(13) Uani 1 1 d . . . . .
H4A H 0.177091 0.231980 0.400673 0.057 Uiso 1 1 calc R U . . .
H4AB H -0.000907 0.119944 0.387146 0.057 Uiso 1 1 calc R U . . .
C5 C -0.0414(9) 0.3067(8) 0.4481(2) 0.0540(15) Uani 1 1 d . . . . .
H5A H -0.171914 0.328547 0.439820 0.065 Uiso 1 1 calc R U . . .
H5AB H -0.032972 0.215401 0.477079 0.065 Uiso 1 1 calc R U . . .
C6 C 0.0424(10) 0.4691(8) 0.4724(2) 0.0577(16) Uani 1 1 d . . . . .
H6A H 0.029964 0.562027 0.444135 0.069 Uiso 1 1 calc R U . . .
H6AB H 0.173689 0.448951 0.479757 0.069 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
Cu1 Cl3 2.2891(12) . ?
Cu1 Cl1 2.2905(12) . ?
Cu1 Cl4 2.3031(12) . ?
Cu1 Cl2 2.3093(12) . ?
N1 C1 1.495(7) . ?
N1 H1NA 0.8900 . ?
N1 H1NB 0.8900 . ?
N1 H1NC 0.8900 . ?
N2 C4 1.484(6) . ?
N2 H2NA 0.8900 . ?
N2 H2NB 0.8900 . ?
N2 H2NC 0.8900 . ?
C1 C2 1.445(8) . ?
C1 H1A 0.9700 . ?
C1 H1AB 0.9700 . ?
C2 C3 1.536(9) . ?
C2 H2A 0.9700 . ?
C2 H2AB 0.9700 . ?
C3 C3 1.517(13) 3_676 ?
C3 H3A 0.9700 . ?
C3 H3AB 0.9700 . ?
C4 C5 1.508(8) . ?
C4 H4A 0.9700 . ?
C4 H4AB 0.9700 . ?
C5 C6 1.481(8) . ?
C5 H5A 0.9700 . ?
C5 H5AB 0.9700 . ?
C6 C6 1.517(11) 3_566 ?
C6 H6A 0.9700 . ?
C6 H6AB 0.9700 . ?

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
Cl3 Cu1 Cl1 179.83(5) . . ?
Cl3 Cu1 Cl4 89.51(4) . . ?
Cl1 Cu1 Cl4 90.47(4) . . ?
Cl3 Cu1 Cl2 90.27(4) . . ?
Cl1 Cu1 Cl2 89.74(5) . . ?
Cl4 Cu1 Cl2 179.71(5) . . ?
C1 N1 H1NA 109.5 . . ?
C1 N1 H1NB 109.5 . . ?
H1NA N1 H1NB 109.5 . . ?
C1 N1 H1NC 109.5 . . ?
H1NA N1 H1NC 109.5 . . ?
H1NB N1 H1NC 109.5 . . ?
C4 N2 H2NA 109.5 . . ?
C4 N2 H2NB 109.5 . . ?
H2NA N2 H2NB 109.5 . . ?
C4 N2 H2NC 109.5 . . ?
H2NA N2 H2NC 109.5 . . ?
H2NB N2 H2NC 109.5 . . ?
C2 C1 N1 113.9(6) . . ?
C2 C1 H1A 108.8 . . ?
N1 C1 H1A 108.8 . . ?
C2 C1 H1AB 108.8 . . ?
N1 C1 H1AB 108.8 . . ?
H1A C1 H1AB 107.7 . . ?
C1 C2 C3 111.1(6) . . ?
C1 C2 H2A 109.4 . . ?
C3 C2 H2A 109.4 . . ?
C1 C2 H2AB 109.4 . . ?
C3 C2 H2AB 109.4 . . ?
H2A C2 H2AB 108.0 . . ?
C3 C3 C2 115.7(7) 3_676 . ?
C3 C3 H3A 108.4 3_676 . ?
C2 C3 H3A 108.4 . . ?
C3 C3 H3AB 108.4 3_676 . ?
C2 C3 H3AB 108.4 . . ?
H3A C3 H3AB 107.4 . . ?
N2 C4 C5 114.0(5) . . ?
N2 C4 H4A 108.7 . . ?
C5 C4 H4A 108.7 . . ?
N2 C4 H4AB 108.7 . . ?
C5 C4 H4AB 108.7 . . ?
H4A C4 H4AB 107.6 . . ?
C6 C5 C4 115.7(5) . . ?
C6 C5 H5A 108.4 . . ?
C4 C5 H5A 108.4 . . ?
C6 C5 H5AB 108.4 . . ?
C4 C5 H5AB 108.4 . . ?
H5A C5 H5AB 107.4 . . ?
C5 C6 C6 114.4(7) . 3_566 ?
C5 C6 H6A 108.7 . . ?
C6 C6 H6A 108.7 3_566 . ?
C5 C6 H6AB 108.7 . . ?
C6 C6 H6AB 108.7 3_566 . ?
H6A C6 H6AB 107.6 . . ?

_refine_diff_density_max         2.295
_refine_diff_density_min         -0.571
_refine_diff_density_rms         0.140


_vrf_PLAT094_C6CuCl4_300K        
; 
RESPONSE: The crystal showed strong diffuse scattering in the 
form of diffuse Bragg peaks and scattering between them. 
As the model dose not account for this type of disorder.
;
