Practical synthesis of ferrocenyldiarylstibines and bismuthines.
Rezazgui, David; Schulz, Jiří; Štěpnička, Petr; Chemical communications (Cambridge, England) 61 (2025) 18705–18708; doi:10.1039/d5cc05762k

data_7135210
_publ_section_title
;
 Practical synthesis of ferrocenyldiarylstibines and bismuthines.
;
_journal_issue                   94
_journal_name_full               'Chemical communications (Cambridge, England)'
_journal_page_first              18705
_journal_page_last               18708
_journal_paper_doi               10.1039/d5cc05762k
_journal_volume                  61
_journal_year                    2025
_chemical_formula_moiety         'C24 H17 F6 Fe Sb'
_chemical_formula_sum            'C24 H17 F6 Fe Sb'
_chemical_formula_weight         596.97
_space_group_crystal_system      monoclinic
_space_group_IT_number           14
_space_group_name_Hall           '-P 2ybc'
_space_group_name_H-M_alt        'P 1 21/c 1'
_atom_sites_solution_hydrogens   geom
_atom_sites_solution_primary     'Intrinsic Phasing'
_audit_creation_method
;FinalCif 2024.9-1 by Daniel Kratzert, Freiburg 2025, 
https://dkratzert.de/finalcif.html
;
_audit_update_record
;
2025-09-25 deposited with the CCDC.	2025-10-23 downloaded from the CCDC.
;
_cell_angle_alpha                90
_cell_angle_beta                 103.8950(10)
_cell_angle_gamma                90
_cell_formula_units_Z            4
_cell_length_a                   11.2444(3)
_cell_length_b                   20.5216(5)
_cell_length_c                   9.9176(3)
_cell_measurement_reflns_used    1046
_cell_measurement_temperature    220(2)
_cell_measurement_theta_max      19.8951
_cell_measurement_theta_min      2.3504
_cell_measurement_wavelength     0.71073
_cell_volume                     2221.55(11)
_computing_cell_refinement       'SAINT V8.41 (Bruker AXS LLC)'
_computing_data_collection       'Bruker Instrument Service v8.5.1.2.Release'
_computing_data_reduction        'SAINT V8.41 (Bruker AXS LLC)'
_computing_molecular_graphics    'shelXle (C.B. Huebschle, rev 1503)'
_computing_structure_refinement  'SHELXL-2019/2 (Sheldrick, 2019)'
_computing_structure_solution    'SHELXT 2018/2 (Sheldrick, 2018)'
_diffrn_ambient_temperature      220(2)
_diffrn_detector_area_resol_mean 7.391
_diffrn_measured_fraction_theta_full 0.997
_diffrn_measured_fraction_theta_max 0.985
_diffrn_measurement_device       'KAPPA diffractometer'
_diffrn_measurement_device_type  'Bruker D8 QUEST'
_diffrn_measurement_method       '\w and \f scans'
_diffrn_radiation_monochromator  'multilayer mirror'
_diffrn_radiation_type           MoK\a
_diffrn_radiation_wavelength     0.71073
_diffrn_reflns_av_R_equivalents  0.0567
_diffrn_reflns_av_unetI/netI     0.0592
_diffrn_reflns_Laue_measured_fraction_full 0.997
_diffrn_reflns_Laue_measured_fraction_max 0.985
_diffrn_reflns_limit_h_max       12
_diffrn_reflns_limit_h_min       -14
_diffrn_reflns_limit_k_max       26
_diffrn_reflns_limit_k_min       -26
_diffrn_reflns_limit_l_max       12
_diffrn_reflns_limit_l_min       -12
_diffrn_reflns_number            15630
_diffrn_reflns_point_group_measured_fraction_full 0.997
_diffrn_reflns_point_group_measured_fraction_max 0.985
_diffrn_reflns_theta_full        25.242
_diffrn_reflns_theta_max         27.482
_diffrn_reflns_theta_min         1.866
_diffrn_source                   'microfocus sealed tube'
_diffrn_source_current           1.0
_diffrn_source_target            Mo
_diffrn_source_type              'INCOATEC I\mS'
_diffrn_source_voltage           50.0
_exptl_absorpt_coefficient_mu    1.928
_exptl_absorpt_correction_T_max  0.828
_exptl_absorpt_correction_T_min  0.534
_exptl_absorpt_correction_type   multi-scan
_exptl_absorpt_process_details
;Krause, L., Herbst-Irmer, R., Sheldrick, G. M., Stalke, D. (2015).
"Comparison of silver and molybdenum microfocus X-ray sources for single-crystal
 structure determination"
J. Appl. Cryst. 48, 3-10.
doi:10.1107/S1600576714022985
;
_exptl_crystal_colour            'translucent pale yellow'
_exptl_crystal_density_diffrn    1.785
_exptl_crystal_description       block
_exptl_crystal_F_000             1168
_exptl_crystal_size_max          0.372
_exptl_crystal_size_mid          0.246
_exptl_crystal_size_min          0.102
_refine_diff_density_max         1.642
_refine_diff_density_min         -1.028
_refine_diff_density_rms         0.122
_refine_ls_extinction_method     none
_refine_ls_goodness_of_fit_ref   1.141
_refine_ls_hydrogen_treatment    constr
_refine_ls_matrix_type           full
_refine_ls_number_parameters     322
_refine_ls_number_reflns         5028
_refine_ls_number_restraints     66
_refine_ls_restrained_S_all      1.159
_refine_ls_R_factor_all          0.0877
_refine_ls_R_factor_gt           0.0717
_refine_ls_shift/su_max          0.001
_refine_ls_shift/su_mean         0.000
_refine_ls_structure_factor_coef Fsqd
_refine_ls_weighting_details
'w=1/[\s^2^(Fo^2^)+16.4459P] where P=(Fo^2^+2Fc^2^)/3'
_refine_ls_weighting_scheme      calc
_refine_ls_wR_factor_gt          0.1476
_refine_ls_wR_factor_ref         0.1543
_reflns_Friedel_coverage         0.000
_reflns_number_gt                4044
_reflns_number_total             5028
_reflns_threshold_expression     'I > 2\s(I)'
_cod_data_source_file            d5cc05762k3.cif
_cod_data_source_block           8
_cod_depositor_comments
;
The following automatic conversions were performed:

data item '_exptl_absorpt_correction_type' value 'Multi-Scan' was
changed to 'multi-scan' in accordance with the
/home/data/users/saulius/crontab/automatic-downloads/current/RSC/lib/dictionaries/cif_core.dic
dictionary named 'cif_core.dic' version 2.4.2 last updated on
2011-04-26.

Automatic conversion script
Id: cif_fix_values 8170 2020-07-09 18:12:32Z antanas 
;
_cod_original_sg_symbol_H-M      'P 21/c'
_cod_database_code               7135210
_shelx_shelxl_version_number     2019/3
_shelx_estimated_absorpt_t_min   0.534
_shelx_estimated_absorpt_t_max   0.828
_computing_bruker_data_scaling
'SADABS-2016/2 - Bruker AXS area detector scaling and absorption correction'
_geom_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.
;
_shelx_res_checksum              38876
_shelx_hkl_checksum              110