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

####################################################################### 
# 
# 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_1
_database_code_depnum_ccdc_archive 'CCDC 1458565'
_audit_update_record             
;
2016-04-20 deposited with the CCDC.
2016-04-25 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         ?
_chemical_formula_sum            'C32.20 H39.80 Cd N10.40 O8.40'
_chemical_formula_weight         819.34

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'
N N 0.0061 0.0033 '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'
Cd Cd -0.8075 1.2024 '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'

_space_group_crystal_system      monoclinic
_space_group_IT_number           14
_space_group_name_H-M_alt        'P 21/c'
_space_group_name_Hall           '-P 2ybc'

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

_cell_length_a                   21.563(5)
_cell_length_b                   14.172(5)
_cell_length_c                   13.642(5)
_cell_angle_alpha                90
_cell_angle_beta                 106.815(5)
_cell_angle_gamma                90
_cell_volume                     3991(2)
_cell_formula_units_Z            4
_cell_measurement_temperature    296(2)
_cell_measurement_reflns_used    22494
_cell_measurement_theta_min      1.743
_cell_measurement_theta_max      24.998

_exptl_crystal_description       block
_exptl_crystal_colour            colorless
_exptl_crystal_density_meas      ?
_exptl_crystal_density_method    ?
_exptl_crystal_density_diffrn    1.364
_exptl_crystal_F_000             1684
_exptl_transmission_factor_min   ?
_exptl_transmission_factor_max   ?
_exptl_crystal_size_max          0.250
_exptl_crystal_size_mid          0.240
_exptl_crystal_size_min          0.200
_exptl_absorpt_coefficient_mu    0.607
_shelx_estimated_absorpt_T_min   0.863
_shelx_estimated_absorpt_T_max   0.888
_exptl_absorpt_correction_type   multi-scan
_exptl_absorpt_correction_T_min  0.864
_exptl_absorpt_correction_T_max  0.890
_exptl_absorpt_process_details   'SADABS 2014/4 Bruker AXS Madison WI USA'
_exptl_absorpt_special_details   ?
_diffrn_ambient_temperature      296(2)
_diffrn_radiation_wavelength     0.71069
_diffrn_radiation_type           MoK\a
_diffrn_source                   'fine-focus sealed tube'
_diffrn_measurement_device_type  'Bruker Smart Apex II CCD'
_diffrn_measurement_method       ω-2θ
_diffrn_detector_area_resol_mean 0.01
_diffrn_reflns_number            22494
_diffrn_reflns_av_unetI/netI     0.0604
_diffrn_reflns_av_R_equivalents  0.0541
_diffrn_reflns_limit_h_min       -24
_diffrn_reflns_limit_h_max       25
_diffrn_reflns_limit_k_min       -16
_diffrn_reflns_limit_k_max       16
_diffrn_reflns_limit_l_min       -16
_diffrn_reflns_limit_l_max       16
_diffrn_reflns_theta_min         1.743
_diffrn_reflns_theta_max         24.998
_diffrn_reflns_theta_full        24.998
_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             7017
_reflns_number_gt                5178
_reflns_threshold_expression     'I > 2σ(I)'
_reflns_Friedel_coverage         0.000
_reflns_Friedel_fraction_max     .
_reflns_Friedel_fraction_full    .

_reflns_special_details          
;
In the single crystal of 1, some residual electron densities, which should be 
 considered as peaks from heavily disordered solvent molecules , 
 did not give a chemical meaningful result after a careful refinement. Therefore,
 the contributions of the disordered solvent molecules were removed
 from the diffraction data using the SQUEEZE routine of PLATON software and then 
 final refinements were carried out. The final platon.sqf file was attached to the 
 CIF file and the electron numbers in the void obtained from the platon.sqf file has
 been used to calculate the guest solvent molecules crystallizing in the pore of 1. 
 These molecules are further estimated by TGA analysis combining with element 
 analysis, and the results were introduced to the formula directly. The H atoms are 
 directly added into the final molecular formula, too. The addition of the solvent and 
 H atoms to the formula unit generates a significant A-level  errors (e.g. density, 
 chemical formula, density) in the final CIF output.
 Reflections were merged by SHELXL according to the crystal
 class for the calculation of statistics and refinement.
 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.
1. Fixed Uiso
 At 1.2 times of:
  All C(H) groups
2. Uiso/Uaniso restraints and constraints
C1 ∼ C2 ∼ C3 ∼ C4 ∼ C5 ∼ C6 ∼ C7 ∼ C8 ∼ C9
∼ C10 ∼ C11 ∼ C12 ∼ C13 ∼ C14 ∼ C15 ∼ C16 ∼ C17
∼ C18 ∼ C19 ∼ C20 ∼ C21 ∼ C22: within 3.8A with sigma of
0.01 and sigma for terminal atoms of 0.03
3.a Aromatic/amide H refined with riding coordinates:
 C3(H3), C4(H4), C6(H6), C7(H7), C8(H8), C9(H9), C10(H10), C12(H12), C14(H14),
 C16(H16), C17(H17), C18(H18), C19(H19), C20(H20), C21(H21), C22(H22)

;

# SQUEEZE RESULTS (Version = 301115)
# Note: Data are Listed for all Voids in the P1 Unit Cell
# i.e. Centre of Gravity, Solvent Accessible Volume,
# Recovered number of Electrons in the Void and
# Details about the Squeezed Material
loop_
_platon_squeeze_void_nr
_platon_squeeze_void_average_x
_platon_squeeze_void_average_y
_platon_squeeze_void_average_z
_platon_squeeze_void_volume
_platon_squeeze_void_count_electrons
_platon_squeeze_void_content
1 0.500 0.280 0.089 2075 537 ' '
_platon_squeeze_void_probe_radius 1.20
_platon_squeeze_details          
;
The PLATON SQUEEZE procedure was used to treat regions of
diffuse solvent which could not be sensibly modelled
in terms of atomic sites. Their contribution to the
diffraction pattern was removed and modified F(obs)**2
written to a new HKL file. The number of electrons thus located,
537 per unit cell, is included in the formula, formula weight,
calculated density, and F(000). This residual electron density
was assigned to 3.4 DMF molecules, as DMF has 
40 electronsthus,134.25/40 = 3.4 . (C2/c system Z=4, 537/4=134.25)
;

_computing_data_collection       'Bruker APEX 2'
_computing_cell_refinement       'Bruker SAINT v8.34a'
_computing_data_reduction        'Bruker SAINT v8.34a'
_computing_structure_solution    'Bruker SHELXTL 2014/4'
_computing_structure_refinement  'SHELXL-2014/7 (Sheldrick, 2014)'
_computing_molecular_graphics    'Bruker SHELXTL'
_computing_publication_material  'Bruker SHELXTL & local programs'
_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)+(0.0418P)²] 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         7017
_refine_ls_number_parameters     316
_refine_ls_number_restraints     390
_refine_ls_R_factor_all          0.0545
_refine_ls_R_factor_gt           0.0373
_refine_ls_wR_factor_ref         0.0935
_refine_ls_wR_factor_gt          0.0904
_refine_ls_goodness_of_fit_ref   1.040
_refine_ls_restrained_S_all      1.072
_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
Cd1 Cd 0.87409(2) 0.44903(2) 0.61063(2) 0.03196(9) Uani 1 1 d . . . . .
C1 C 0.7434(2) 0.4708(3) 0.5795(4) 0.0640(11) Uani 1 1 d . U . . .
C2 C 0.6714(2) 0.4785(3) 0.5555(4) 0.0730(12) Uani 1 1 d . U . . .
C3 C 0.6322(2) 0.4049(4) 0.5223(5) 0.0975(15) Uani 1 1 d . U . . .
H3A H 0.6502 0.3471 0.5134 0.117 Uiso 1 1 calc R U . . .
C4 C 0.5643(2) 0.4120(4) 0.5001(5) 0.1026(15) Uani 1 1 d . U . . .
H4A H 0.5386 0.3591 0.4777 0.123 Uiso 1 1 calc R U . . .
C5 C 0.5361(2) 0.4957(4) 0.5114(5) 0.0854(14) Uani 1 1 d . U . . .
C6 C 0.5758(2) 0.5690(4) 0.5462(5) 0.1002(15) Uani 1 1 d . U . . .
H6A H 0.5579 0.6261 0.5580 0.120 Uiso 1 1 calc R U . . .
C7 C 0.6423(2) 0.5628(4) 0.5652(5) 0.0992(15) Uani 1 1 d . U . . .
H7A H 0.6677 0.6165 0.5848 0.119 Uiso 1 1 calc R U . . .
C8 C 0.90187(19) 0.6714(2) 0.6475(3) 0.0425(8) Uani 1 1 d . U . . .
H8A H 0.8643 0.6781 0.6673 0.051 Uiso 1 1 calc R U . . .
C9 C 0.98101(19) 0.6116(3) 0.6068(3) 0.0503(10) Uani 1 1 d . U . . .
H9A H 1.0094 0.5674 0.5935 0.060 Uiso 1 1 calc R U . . .
C10 C 0.98684(19) 0.7054(3) 0.6001(3) 0.0517(9) Uani 1 1 d . U . . .
H10A H 1.0189 0.7378 0.5806 0.062 Uiso 1 1 calc R U . . .
C11 C 0.91871(17) 0.8414(2) 0.6243(3) 0.0360(7) Uani 1 1 d . U . . .
C12 C 0.89886(17) 0.8791(2) 0.7027(3) 0.0375(8) Uani 1 1 d . U . . .
H12A H 0.8967 0.8421 0.7580 0.045 Uiso 1 1 calc R U . . .
C13 C 0.88213(17) 0.9735(2) 0.6975(2) 0.0361(8) Uani 1 1 d . U . . .
C14 C 0.88355(18) 1.0287(2) 0.6142(3) 0.0410(8) Uani 1 1 d . U . . .
H14A H 0.8732 1.0925 0.6122 0.049 Uiso 1 1 calc R U . . .
C15 C 0.90076(18) 0.9867(2) 0.5335(3) 0.0387(8) Uani 1 1 d . U . . .
C16 C 0.91953(17) 0.8937(2) 0.5386(3) 0.0394(8) Uani 1 1 d . U . . .
H16A H 0.9325 0.8663 0.4857 0.047 Uiso 1 1 calc R U . . .
C17 C 0.9104(2) 1.0121(3) 0.3576(3) 0.0467(9) Uani 1 1 d . U . . .
H17A H 0.9317 0.9560 0.3526 0.056 Uiso 1 1 calc R U . . .
C18 C 0.8638(2) 1.1442(3) 0.3217(3) 0.0627(11) Uani 1 1 d . U . . .
H18A H 0.8459 1.1981 0.2857 0.075 Uiso 1 1 calc R U . . .
C19 C 0.8658(2) 1.1257(3) 0.4188(3) 0.0621(11) Uani 1 1 d . U . . .
H19A H 0.8502 1.1639 0.4618 0.075 Uiso 1 1 calc R U . . .
C20 C 0.8276(2) 1.0970(3) 0.7751(3) 0.0548(10) Uani 1 1 d . U . . .
H20A H 0.8091 1.1336 0.7175 0.066 Uiso 1 1 calc R U . . .
C21 C 0.87914(18) 0.9868(2) 0.8774(3) 0.0362(8) Uani 1 1 d . U . . .
H21A H 0.9030 0.9326 0.9015 0.043 Uiso 1 1 calc R U . . .
C22 C 0.8251(2) 1.1127(3) 0.8703(3) 0.0548(10) Uani 1 1 d . U . . .
H22A H 0.8042 1.1637 0.8899 0.066 Uiso 1 1 calc R U . . .
N1 N 0.92721(14) 0.59053(19) 0.6360(2) 0.0389(7) Uani 1 1 d . . . . .
N2 N 0.93608(14) 0.74387(18) 0.6276(2) 0.0351(7) Uani 1 1 d . . . . .
N3 N 0.86343(14) 1.01504(18) 0.7792(2) 0.0354(7) Uani 1 1 d . . . . .
N4 N 0.85757(14) 1.04302(19) 0.9353(2) 0.0383(7) Uani 1 1 d . . . . .
N5 N 0.89508(16) 1.04022(18) 0.4424(2) 0.0421(8) Uani 1 1 d . . . . .
N6 N 0.89170(16) 1.07313(19) 0.2841(2) 0.0455(8) Uani 1 1 d . . . . .
N7 N 0.95849(17) 0.2886(2) 0.6152(2) 0.0459(8) Uani 1 1 d . . . . .
O1 O 0.76733(13) 0.3918(2) 0.5727(2) 0.0601(7) Uani 1 1 d . . . . .
O2 O 0.77637(14) 0.5426(2) 0.6020(3) 0.0731(9) Uani 1 1 d . . . . .
O3 O 0.89977(14) 0.27835(17) 0.6107(2) 0.0513(7) Uani 1 1 d . . . . .
O4 O 0.97877(12) 0.37226(18) 0.6147(2) 0.0532(7) Uani 1 1 d . . . . .
O5 O 0.99436(15) 0.2207(2) 0.6199(2) 0.0734(9) Uani 1 1 d . . . . .


_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
Cd1 N1 2.286(3) . ?
Cd1 N6 2.307(3) 4_576 ?
Cd1 N4 2.316(3) 4_575 ?
Cd1 O1 2.353(3) . ?
Cd1 O2 2.463(3) . ?
Cd1 O3 2.481(3) . ?
Cd1 O4 2.492(3) . ?
Cd1 C1 2.743(4) . ?
C1 O2 1.228(5) . ?
C1 O1 1.248(5) . ?
C1 C2 1.495(6) . ?
C2 C3 1.337(7) . ?
C2 C7 1.374(6) . ?
C3 C4 1.410(6) . ?
C3 H3A 0.9300 . ?
C4 C5 1.362(7) . ?
C4 H4A 0.9300 . ?
C5 C6 1.343(7) . ?
C5 C5 1.503(9) 3_666 ?
C6 C7 1.385(7) . ?
C6 H6A 0.9300 . ?
C7 H7A 0.9300 . ?
C8 N1 1.298(4) . ?
C8 N2 1.338(4) . ?
C8 H8A 0.9300 . ?
C9 C10 1.340(5) . ?
C9 N1 1.364(4) . ?
C9 H9A 0.9300 . ?
C10 N2 1.369(4) . ?
C10 H10A 0.9300 . ?
C11 C12 1.371(4) . ?
C11 C16 1.389(4) . ?
C11 N2 1.429(4) . ?
C12 C13 1.382(4) . ?
C12 H12A 0.9300 . ?
C13 C14 1.388(4) . ?
C13 N3 1.418(4) . ?
C14 C15 1.393(4) . ?
C14 H14A 0.9300 . ?
C15 C16 1.375(5) . ?
C15 N5 1.430(4) . ?
C16 H16A 0.9300 . ?
C17 N6 1.297(4) . ?
C17 N5 1.352(4) . ?
C17 H17A 0.9300 . ?
C18 C19 1.338(5) . ?
C18 N6 1.349(4) . ?
C18 H18A 0.9300 . ?
C19 N5 1.361(4) . ?
C19 H19A 0.9300 . ?
C20 C22 1.334(5) . ?
C20 N3 1.386(4) . ?
C20 H20A 0.9300 . ?
C21 N4 1.299(4) . ?
C21 N3 1.345(4) . ?
C21 H21A 0.9300 . ?
C22 N4 1.377(4) . ?
C22 H22A 0.9300 . ?
N4 Cd1 2.316(3) 4_576 ?
N6 Cd1 2.307(3) 4_575 ?
N7 O5 1.225(4) . ?
N7 O3 1.258(4) . ?
N7 O4 1.264(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
N1 Cd1 N6 92.14(10) . 4_576 ?
N1 Cd1 N4 91.97(10) . 4_575 ?
N6 Cd1 N4 174.92(10) 4_576 4_575 ?
N1 Cd1 O1 138.72(10) . . ?
N6 Cd1 O1 92.23(11) 4_576 . ?
N4 Cd1 O1 86.64(10) 4_575 . ?
N1 Cd1 O2 85.37(10) . . ?
N6 Cd1 O2 90.41(11) 4_576 . ?
N4 Cd1 O2 92.89(11) 4_575 . ?
O1 Cd1 O2 53.57(10) . . ?
N1 Cd1 O3 138.87(10) . . ?
N6 Cd1 O3 84.05(9) 4_576 . ?
N4 Cd1 O3 90.89(9) 4_575 . ?
O1 Cd1 O3 82.41(10) . . ?
O2 Cd1 O3 135.43(10) . . ?
N1 Cd1 O4 88.20(10) . . ?
N6 Cd1 O4 92.20(10) 4_576 . ?
N4 Cd1 O4 84.95(9) 4_575 . ?
O1 Cd1 O4 132.58(9) . . ?
O2 Cd1 O4 173.15(10) . . ?
O3 Cd1 O4 51.23(9) . . ?
N1 Cd1 C1 111.85(12) . . ?
N6 Cd1 C1 91.77(13) 4_576 . ?
N4 Cd1 C1 89.47(13) 4_575 . ?
O1 Cd1 C1 26.98(11) . . ?
O2 Cd1 C1 26.59(11) . . ?
O3 Cd1 C1 109.20(12) . . ?
O4 Cd1 C1 159.39(12) . . ?
O2 C1 O1 122.7(4) . . ?
O2 C1 C2 119.0(4) . . ?
O1 C1 C2 118.3(4) . . ?
O2 C1 Cd1 63.9(2) . . ?
O1 C1 Cd1 58.8(2) . . ?
C2 C1 Cd1 175.8(4) . . ?
C3 C2 C7 116.7(4) . . ?
C3 C2 C1 122.2(4) . . ?
C7 C2 C1 121.1(4) . . ?
C2 C3 C4 122.2(5) . . ?
C2 C3 H3A 118.9 . . ?
C4 C3 H3A 118.9 . . ?
C5 C4 C3 120.5(5) . . ?
C5 C4 H4A 119.8 . . ?
C3 C4 H4A 119.8 . . ?
C6 C5 C4 117.1(4) . . ?
C6 C5 C5 121.8(6) . 3_666 ?
C4 C5 C5 121.1(6) . 3_666 ?
C5 C6 C7 122.5(5) . . ?
C5 C6 H6A 118.8 . . ?
C7 C6 H6A 118.8 . . ?
C2 C7 C6 120.9(5) . . ?
C2 C7 H7A 119.5 . . ?
C6 C7 H7A 119.5 . . ?
N1 C8 N2 112.2(3) . . ?
N1 C8 H8A 123.9 . . ?
N2 C8 H8A 123.9 . . ?
C10 C9 N1 110.0(3) . . ?
C10 C9 H9A 125.0 . . ?
N1 C9 H9A 125.0 . . ?
C9 C10 N2 106.1(3) . . ?
C9 C10 H10A 126.9 . . ?
N2 C10 H10A 126.9 . . ?
C12 C11 C16 122.2(3) . . ?
C12 C11 N2 119.4(3) . . ?
C16 C11 N2 118.4(3) . . ?
C11 C12 C13 118.2(3) . . ?
C11 C12 H12A 120.9 . . ?
C13 C12 H12A 120.9 . . ?
C12 C13 C14 121.4(3) . . ?
C12 C13 N3 119.4(3) . . ?
C14 C13 N3 119.2(3) . . ?
C13 C14 C15 118.8(3) . . ?
C13 C14 H14A 120.6 . . ?
C15 C14 H14A 120.6 . . ?
C16 C15 C14 120.7(3) . . ?
C16 C15 N5 120.2(3) . . ?
C14 C15 N5 119.0(3) . . ?
C15 C16 C11 118.6(3) . . ?
C15 C16 H16A 120.7 . . ?
C11 C16 H16A 120.7 . . ?
N6 C17 N5 111.5(3) . . ?
N6 C17 H17A 124.2 . . ?
N5 C17 H17A 124.2 . . ?
C19 C18 N6 109.9(3) . . ?
C19 C18 H18A 125.1 . . ?
N6 C18 H18A 125.1 . . ?
C18 C19 N5 106.8(3) . . ?
C18 C19 H19A 126.6 . . ?
N5 C19 H19A 126.6 . . ?
C22 C20 N3 106.3(3) . . ?
C22 C20 H20A 126.9 . . ?
N3 C20 H20A 126.9 . . ?
N4 C21 N3 113.1(3) . . ?
N4 C21 H21A 123.5 . . ?
N3 C21 H21A 123.5 . . ?
C20 C22 N4 110.5(3) . . ?
C20 C22 H22A 124.7 . . ?
N4 C22 H22A 124.7 . . ?
C8 N1 C9 105.4(3) . . ?
C8 N1 Cd1 125.6(2) . . ?
C9 N1 Cd1 125.4(2) . . ?
C8 N2 C10 106.3(3) . . ?
C8 N2 C11 126.5(3) . . ?
C10 N2 C11 126.8(3) . . ?
C21 N3 C20 105.4(3) . . ?
C21 N3 C13 127.8(3) . . ?
C20 N3 C13 126.7(3) . . ?
C21 N4 C22 104.7(3) . . ?
C21 N4 Cd1 133.0(2) . 4_576 ?
C22 N4 Cd1 121.9(2) . 4_576 ?
C17 N5 C19 105.7(3) . . ?
C17 N5 C15 127.3(3) . . ?
C19 N5 C15 126.5(3) . . ?
C17 N6 C18 106.1(3) . . ?
C17 N6 Cd1 128.6(2) . 4_575 ?
C18 N6 Cd1 122.2(3) . 4_575 ?
O5 N7 O3 121.5(3) . . ?
O5 N7 O4 121.6(3) . . ?
O3 N7 O4 117.0(3) . . ?
C1 O1 Cd1 94.2(3) . . ?
C1 O2 Cd1 89.5(3) . . ?
N7 O3 Cd1 96.2(2) . . ?
N7 O4 Cd1 95.6(2) . . ?

_refine_diff_density_max         0.600
_refine_diff_density_min         -0.483
_refine_diff_density_rms         0.068

