Desymmetrization Reactions of Indigo with Grignard Reagents for the Synthesis of Selective Antiplasmodial [1<i>H</i>,3'<i>H</i>]-3-Aryl-2,2'-diindol-3'-ones.
Butler, Nicholas M.; Bremner, John B.; Willis, Anthony C.; Lucantoni, Leonardo; Avery, Vicky M.; Keller, Paul A.; The Journal of organic chemistry 84 (2019) 11228–11239; doi:10.1021/acs.joc.9b01442

data_4033865
_publ_section_title
;
 Desymmetrization Reactions of Indigo with Grignard Reagents for the
 Synthesis of Selective Antiplasmodial
 [1<i>H</i>,3'<i>H</i>]-3-Aryl-2,2'-diindol-3'-ones.
;
_journal_issue                   17
_journal_name_full               'The Journal of organic chemistry'
_journal_page_first              11228
_journal_page_last               11239
_journal_paper_doi               10.1021/acs.joc.9b01442
_journal_volume                  84
_journal_year                    2019
_chemical_absolute_configuration ad
_chemical_compound_source        ' from U of Wollongong'
_chemical_formula_moiety         'C27 H21 Cl1 N2 O3'
_chemical_formula_sum            'C27 H21 Cl N2 O3'
_chemical_formula_weight         456.93
_space_group_IT_number           33
_space_group_name_Hall           'P 2c -2n'
_space_group_name_H-M_alt        'P n a 21'
_symmetry_cell_setting           orthorhombic
_symmetry_space_group_name_Hall  'P 2c -2n'
_symmetry_space_group_name_H-M   'P n a 21'
_atom_sites_solution_hydrogens   difmap
_atom_sites_solution_primary     direct
_audit_creation_date             17-10-20
_audit_creation_method           CRYSTALS_ver_14.40
_audit_update_record
;
2017-10-20 - Report on C27 H21 Cl1 N2 O3 
             by Anthony C. Willis
             for Paul Keller

2017-10-20 - details of refinement in _refine_special_details below

2017-10-20 - passes checkcif tests with no significant warnings  
;
_cell_angle_alpha                90
_cell_angle_beta                 90
_cell_angle_gamma                90
_cell_formula_units_Z            4
_cell_length_a                   18.76631(12)
_cell_length_b                   14.88559(11)
_cell_length_c                   7.88336(7)
_cell_measurement_reflns_used    20999
_cell_measurement_temperature    150
_cell_measurement_theta_max      74
_cell_measurement_theta_min      2
_cell_volume                     2202.20(3)
_computing_cell_refinement       'CrysAlisPro 1.171.38.46 (Rigaku OD, 2017)'
_computing_data_collection       'CrysAlisPro 1.171.38.46 (Rigaku OD, 2017)'
_computing_data_reduction        'CrysAlisPro 1.171.38.46 (Rigaku OD, 2017)'
_computing_molecular_graphics    'PLATON (Spek, 2008)'
_computing_publication_material  'CRYSTALS (Betteridge et al., 2003)'
_computing_structure_refinement  'CRYSTALS (Betteridge et al., 2003)'
_computing_structure_solution    'SIR92 (Altomare et al., 1994)'
_diffrn_ambient_environment      N~2~
_diffrn_ambient_temperature      150
_diffrn_detector                 'CCD plate'
_diffrn_detector_type            EosS2
_diffrn_measured_fraction_theta_full 0.996
_diffrn_measured_fraction_theta_max 0.996
_diffrn_measurement_device       'four-circle diffractometer'
_diffrn_measurement_device_type  'SuperNova, Dual, Cu at zero, EosS2'
_diffrn_measurement_method       '\w scans'
_diffrn_radiation_monochromator  mirror
_diffrn_radiation_probe          x-ray
_diffrn_radiation_type           'Cu K\a'
_diffrn_radiation_wavelength     1.54184
_diffrn_reflns_av_R_equivalents  0.024
_diffrn_reflns_av_sigmaI/netI    0.0297
_diffrn_reflns_limit_h_max       23
_diffrn_reflns_limit_h_min       -23
_diffrn_reflns_limit_k_max       18
_diffrn_reflns_limit_k_min       -18
_diffrn_reflns_limit_l_max       8
_diffrn_reflns_limit_l_min       -9
_diffrn_reflns_number            34133
_diffrn_reflns_theta_full        73.832
_diffrn_reflns_theta_max         73.832
_diffrn_reflns_theta_min         3.790
_diffrn_source                   'micro-focus sealed X-ray tube'
_diffrn_source_type              'SuperNova (Cu) X-ray Source'
_diffrn_standards_number         0
_exptl_absorpt_coefficient_mu    1.805
_exptl_absorpt_correction_T_max  0.79
_exptl_absorpt_correction_T_min  0.68
_exptl_absorpt_correction_type   multi-scan
_exptl_absorpt_process_details
;
CrysAlisPro version 1.171.38.46 (Rigaku Oxford Diffraction, 2017)
(Release 29 April 2016; compiled 27 May 2016,16:53)
Empirical absorption correction using spherical harmonics,
 implemented in SCALE3 ABSPACK scaling algorithm.
;
_exptl_crystal_colour            orange-red
_exptl_crystal_density_diffrn    1.378
_exptl_crystal_density_method    'not measured'
_exptl_crystal_description       block
_exptl_crystal_F_000             952
_exptl_crystal_size_max          0.339
_exptl_crystal_size_mid          0.204
_exptl_crystal_size_min          0.134
_refine_diff_density_max         0.28
_refine_diff_density_min         -0.65
_refine_ls_abs_structure_details 'Flack (1983), 1749 Friedel-pairs'
_refine_ls_abs_structure_Flack   0.005(13)
_refine_ls_extinction_method     None
_refine_ls_goodness_of_fit_ref   1.0061
_refine_ls_hydrogen_treatment    constr
_refine_ls_matrix_type           full
_refine_ls_number_parameters     299
_refine_ls_number_reflns         4142
_refine_ls_number_restraints     1
_refine_ls_R_factor_all          0.0331
_refine_ls_R_factor_gt           0.0329
_refine_ls_shift/su_max          0.0005453
_refine_ls_shift/su_mean         0.0000709
_refine_ls_structure_factor_coef Fsqd
_refine_ls_weighting_details
;
 Method= Modified Sheldrick 
 w=1/[\s^2^(F^2^) + ( 0.06P)^2^ + 0.54P] 
 ,where P=(max(Fo^2^,0) + 2Fc^2^)/3 
;
_refine_ls_weighting_scheme      calc
_refine_ls_wR_factor_all         0.0897
_refine_ls_wR_factor_gt          0.0895
_refine_ls_wR_factor_ref         0.0897
_reflns_limit_h_max              23
_reflns_limit_h_min              0
_reflns_limit_k_max              18
_reflns_limit_k_min              0
_reflns_limit_l_max              8
_reflns_limit_l_min              -9
_reflns_number_gt                4091
_reflns_number_total             4142
_reflns_threshold_expression     I>2.0\s(I)
_oxford_diffrn_Wilson_B_factor   2.61
_oxford_diffrn_Wilson_scale      0.03
_oxford_refine_ls_r_factor_ref   0.0331
_oxford_refine_ls_scale          5.91(11)
_oxford_reflns_number_all        4142
_oxford_reflns_threshold_expression_ref I>-10.0\s(I)
_oxford_structure_analysis_title 'Z:\kel1709SNQ\Tony_kel1709SNQ_da At 12: 6 on'
_cod_data_source_file            jo9b01442_si_004.cif
_cod_data_source_block           kel1709SNQ
_cod_original_cell_volume        2202.21(3)
_cod_original_sg_symbol_H-M      'P n a 21 '
_cod_original_formula_sum        'C27 H21 Cl1 N2 O3'
_cod_database_code               4033865
_oxdiff_exptl_absorpt_empirical_details
;
Empirical correction (ABSPACK) includes:
- Absorption correction using spherical harmonics
- Frame scaling
;
_iucr_refine_instruction_details_constraints
;
BLOCK SCALE X'S, U'S 
CONT ENANTIO 
RIDE C   (   2,X'S) H   (  21,X'S) 
RIDE C   (   3,X'S) H   (  31,X'S) 
RIDE C   (   4,X'S) H   (  41,X'S) 
RIDE C   (   5,X'S) H   (  51,X'S) 
RIDE C   (  12,X'S) H   ( 121,X'S) 
RIDE C   (  13,X'S) H   ( 131,X'S) 
RIDE C   (  14,X'S) H   ( 141,X'S) 
RIDE C   (  15,X'S) H   ( 151,X'S) 
RIDE C   (  18,X'S) H   ( 181,X'S) 
RIDE C   (  19,X'S) H   ( 191,X'S) 
RIDE C   (  20,X'S) H   ( 201,X'S) 
RIDE C   (  21,X'S) H   ( 211,X'S) 
RIDE C   (  25,X'S) H   ( 251,X'S) H   ( 252,X'S) H   ( 253,X'S) 
RIDE C   (  26,X'S) H   ( 261,X'S) H   ( 262,X'S) H   ( 263,X'S) 
RIDE C   (  27,X'S) H   ( 271,X'S) H   ( 272,X'S) H   ( 273,X'S) 
END                                                                             
;
_iucr_refine_instruction_details_restraints
;
NO 
REM   HREST   START (DO NOT REMOVE THIS LINE) 
REM   HREST   END (DO NOT REMOVE THIS LINE) 
END                                                                             
;