 
data_ANI_1_071122_0m_a
 
_audit_creation_method            'SHELXL-2019/1'
_shelx_SHELXL_version_number      '2019/1'
_chemical_name_systematic         ?
_chemical_name_common             ?
_chemical_melting_point           ?
_chemical_formula_moiety          'C14 H12 N2 O2'
_chemical_formula_sum
 'C14 H12 N2 O2' 
_chemical_formula_weight          240.26

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'
 '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'
 
_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                    5.3310(9)
_cell_length_b                    5.3762(9)
_cell_length_c                    20.182(3)
_cell_angle_alpha                 90
_cell_angle_beta                  93.598(5)
_cell_angle_gamma                 90
_cell_volume                      577.29(17)
_cell_formula_units_Z             2
_cell_measurement_temperature     300(2)
_cell_measurement_reflns_used      6473
_cell_measurement_theta_min        3.83
_cell_measurement_theta_max       28.08
 
_exptl_crystal_description       'block'
_exptl_crystal_colour            'gold'
_exptl_crystal_density_meas       ?
_exptl_crystal_density_method     ?
_exptl_crystal_density_diffrn     1.382          
_exptl_crystal_F_000              252
_exptl_transmission_factor_min    ?
_exptl_transmission_factor_max    ?
_exptl_crystal_size_max           0.300
_exptl_crystal_size_mid           0.220
_exptl_crystal_size_min           0.120
_exptl_absorpt_coefficient_mu     0.094
_shelx_estimated_absorpt_T_min    0.972
_shelx_estimated_absorpt_T_max    0.989
_exptl_absorpt_correction_type    multi-scan
_exptl_absorpt_correction_T_min   0.6861
_exptl_absorpt_correction_T_max   0.7457
_exptl_absorpt_process_details    
;
 SADABS 2016/2: Krause, L., Herbst-Irmer, R., Sheldrick G.M. & Stalke D.,
 J. Appl. Cryst. 48 (2015) 3-10
;
_exptl_absorpt_special_details    ?
_diffrn_ambient_temperature       300(2)
_diffrn_radiation_wavelength      0.71073
_diffrn_radiation_type            MoK\a
_diffrn_source                    'i-mu-s microfocus source'
_diffrn_measurement_device_type   
 'Bruker D8 QUEST diffractometer with PHOTON II detector'
_diffrn_measurement_method        'φ and ω scans'
_diffrn_detector_area_resol_mean  ?
_diffrn_reflns_number             14639
_diffrn_reflns_av_unetI/netI      0.0206
_diffrn_reflns_av_R_equivalents   0.0376
_diffrn_reflns_limit_h_min        -7
_diffrn_reflns_limit_h_max        7
_diffrn_reflns_limit_k_min        -7
_diffrn_reflns_limit_k_max        7
_diffrn_reflns_limit_l_min        -26
_diffrn_reflns_limit_l_max        26
_diffrn_reflns_theta_min          3.899
_diffrn_reflns_theta_max          28.282
_diffrn_reflns_theta_full         25.242
_diffrn_measured_fraction_theta_max   0.990
_diffrn_measured_fraction_theta_full  0.988
_diffrn_reflns_Laue_measured_fraction_max    0.990
_diffrn_reflns_Laue_measured_fraction_full   0.988
_diffrn_reflns_point_group_measured_fraction_max   0.990
_diffrn_reflns_point_group_measured_fraction_full  0.988
_reflns_number_total              1410
_reflns_number_gt                 1147
_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 APEX4'
_computing_cell_refinement       'Bruker APEX4/SAINT'
_computing_data_reduction        'Bruker APEX4/SAINT'
_computing_structure_solution     'SHELXL-2019/1 (Sheldrick, 2019)'
_computing_structure_refinement 'SHELXL-2019/1 (Sheldrick, 2019)'
_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)+(0.0535P)²+0.1355P] 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          1410
_refine_ls_number_parameters      82
_refine_ls_number_restraints      0
_refine_ls_R_factor_all           0.0570
_refine_ls_R_factor_gt            0.0444
_refine_ls_wR_factor_ref          0.1209
_refine_ls_wR_factor_gt           0.1123
_refine_ls_goodness_of_fit_ref    1.072
_refine_ls_restrained_S_all       1.072
_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
O1 O 0.23070(18) 0.1162(2) 0.45667(5) 0.0581(3) Uani 1 1 d . . . . .
N1 N 0.6438(2) 0.2212(2) 0.44924(5) 0.0426(3) Uani 1 1 d . . . . .
H1 H 0.791782 0.186555 0.466173 0.051 Uiso 1 1 calc R U . . .
C1 C 0.6292(2) 0.4070(2) 0.39919(6) 0.0376(3) Uani 1 1 d . . . . .
C2 C 0.8255(3) 0.5756(3) 0.39771(7) 0.0460(3) Uani 1 1 d . . . . .
H2 H 0.960823 0.564988 0.428986 0.055 Uiso 1 1 calc R U . . .
C3 C 0.8203(3) 0.7592(3) 0.34984(8) 0.0518(4) Uani 1 1 d . . . . .
H3 H 0.951594 0.872949 0.349274 0.062 Uiso 1 1 calc R U . . .
C4 C 0.6214(3) 0.7750(3) 0.30276(8) 0.0503(4) Uani 1 1 d . . . . .
H4 H 0.617894 0.898929 0.270561 0.060 Uiso 1 1 calc R U . . .
C5 C 0.4288(3) 0.6059(3) 0.30404(7) 0.0507(4) Uani 1 1 d . . . . .
H5 H 0.295237 0.615938 0.272227 0.061 Uiso 1 1 calc R U . . .
C6 C 0.4295(3) 0.4208(3) 0.35168(7) 0.0454(3) Uani 1 1 d . . . . .
H6 H 0.298026 0.307175 0.351900 0.054 Uiso 1 1 calc R U . . .
C7 C 0.4539(2) 0.0940(2) 0.47304(6) 0.0410(3) 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
O1 C7 1.2207(16) . ?
N1 C7 1.3356(17) . ?
N1 C1 1.4193(16) . ?
N1 H1 0.8600 . ?
C1 C2 1.3862(19) . ?
C1 C6 1.3894(18) . ?
C2 C3 1.380(2) . ?
C2 H2 0.9300 . ?
C3 C4 1.382(2) . ?
C3 H3 0.9300 . ?
C4 C5 1.373(2) . ?
C4 H4 0.9300 . ?
C5 C6 1.3836(19) . ?
C5 H5 0.9300 . ?
C6 H6 0.9300 . ?
C7 C7 1.543(2) 3_656 ?
 
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
C7 N1 C1 127.38(11) . . ?
C7 N1 H1 116.3 . . ?
C1 N1 H1 116.3 . . ?
C2 C1 C6 119.80(12) . . ?
C2 C1 N1 117.89(12) . . ?
C6 C1 N1 122.29(12) . . ?
C3 C2 C1 120.05(13) . . ?
C3 C2 H2 120.0 . . ?
C1 C2 H2 120.0 . . ?
C2 C3 C4 120.42(13) . . ?
C2 C3 H3 119.8 . . ?
C4 C3 H3 119.8 . . ?
C5 C4 C3 119.28(13) . . ?
C5 C4 H4 120.4 . . ?
C3 C4 H4 120.4 . . ?
C4 C5 C6 121.34(13) . . ?
C4 C5 H5 119.3 . . ?
C6 C5 H5 119.3 . . ?
C5 C6 C1 119.11(13) . . ?
C5 C6 H6 120.4 . . ?
C1 C6 H6 120.4 . . ?
O1 C7 N1 126.93(12) . . ?
O1 C7 C7 121.10(15) . 3_656 ?
N1 C7 C7 111.97(14) . 3_656 ?
 
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
C7 N1 C1 C2 157.48(13) . . . . ?
C7 N1 C1 C6 -23.9(2) . . . . ?
C6 C1 C2 C3 1.1(2) . . . . ?
N1 C1 C2 C3 179.78(12) . . . . ?
C1 C2 C3 C4 -0.6(2) . . . . ?
C2 C3 C4 C5 -0.1(2) . . . . ?
C3 C4 C5 C6 0.3(2) . . . . ?
C4 C5 C6 C1 0.2(2) . . . . ?
C2 C1 C6 C5 -0.9(2) . . . . ?
N1 C1 C6 C5 -179.48(13) . . . . ?
C1 N1 C7 O1 -1.0(2) . . . . ?
C1 N1 C7 C7 179.55(13) . . . 3_656 ?
 
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 
 _geom_hbond_publ_flag
N1 H1 O1  0.86 2.39 3.1733(16) 152.0 1_655 yes
N1 H1 O1  0.86 2.26 2.6803(14) 110.0 3_656 yes
C6 H6 O1  0.93 2.40 2.9286(17) 116.0 . yes
 
_refine_diff_density_max    0.255
_refine_diff_density_min   -0.145
_refine_diff_density_rms    0.032



