# Supplementary Material (ESI) for Chemical Communications # This journal is (c) The Royal Society of Chemistry 2011 data_global _journal_coden_Cambridge 182 loop_ _publ_author_name 'Okuma, Kentaro' _publ_contact_author_name 'Okuma, Kentaro' _publ_contact_author_email kokuma@fukuoka-u.ac.jp _publ_section_title ; Reaction of Arynes with Amino Acid Esters ; _publ_contact_author_address ; Department of Chemistry, Fukuoka University ; _publ_contact_author_fax ' ' _publ_contact_author_phone ' ' # Submission details _publ_requested_journal 'Acta Crystallographica Section C ' # Attachment '- full.cif' # CIF Copied by cif2cif, version 0.0.8 - beta ( 2 Apr 98) data_full _database_code_depnum_ccdc_archive 'CCDC 815166' #TrackingRef '- full.cif' _audit_creation_method maXus _publ_section_abstract ; We present the crystal and molecular structure of ; _publ_section_comment ; The study of the titled structure was undertaken to establish its three dimensional structure. Geometries are tabulated below. All diagrams and calculations were performed using maXus (Bruker Nonius, Delft & MacScience, Japan). ; _publ_section_synopsis ; ; _publ_section_exptl_prep ; ; _publ_section_exptl_refinement ; ; _publ_section_figure_captions ; ; _publ_section_acknowledgements ; ; _chemical_compound_source 'Okuma laboratory' _exptl_crystal_description Cube _exptl_crystal_colour Colourless _cell_measurement_temperature 298 _refine_ls_hydrogen_treatment constr _diffrn_measurement_device 'DIP Image plate' _computing_data_collection 'DIP Image plate' _computing_data_reduction 'maXus (Mackay et al., 1999)' _cell_measurement_reflns_used ? _cell_measurement_theta_min ? _cell_measurement_theta_max ? _diffrn_radiation_source 'fine-focus sealed tube' _diffrn_reflns_limit_h_min -13 _diffrn_reflns_limit_h_max 13 _diffrn_reflns_limit_k_min -6 _diffrn_reflns_limit_k_max 3 _diffrn_reflns_limit_l_min -19 _diffrn_reflns_limit_l_max 18 loop_ _diffrn_radiation_wavelength 1.54184 _diffrn_radiation_wavelength_id all _diffrn_orient_matrix_type X=UH _diffrn_orient_matrix_UB_11 -0.07198 _diffrn_orient_matrix_UB_12 -0.02095 _diffrn_orient_matrix_UB_13 0.01918 _diffrn_orient_matrix_UB_21 0.04422 _diffrn_orient_matrix_UB_22 -0.18049 _diffrn_orient_matrix_UB_23 -0.03119 _diffrn_orient_matrix_UB_31 0.00760 _diffrn_orient_matrix_UB_32 -0.01057 _diffrn_orient_matrix_UB_33 0.07192 _cell_formula_units_Z 4 _exptl_crystal_density_diffrn 1.409 _exptl_crystal_density_method 'not measured' _exptl_special_details ; ? ; _chemical_formula_weight 203.197 _diffrn_radiation_type ' CuK\a' loop_ _symmetry_equiv_pos_as_xyz +X,+Y,+Z -X,-Y,-Z '-X,+Y+ 1/2,-Z+ 1/2' '+X,-Y+ 1/2,+Z+ 1/2' _symmetry_space_group_name_H-M 'P 21/c ' _symmetry_cell_setting Monoclinic _chemical_formula_moiety 'C11 H9 N O3 ' _chemical_formula_sum 'C11 H9 N O3 ' _chemical_name_systematic ; ? ; _cell_length_a 13.1450(11) _cell_length_b 5.3200(4) _cell_length_c 17.294(2) _cell_angle_alpha 90.00 _cell_angle_beta 127.636(4) _cell_angle_gamma 90.00 _cell_volume 957.73(14) _diffrn_reflns_number 1507 _diffrn_reflns_theta_max 68.29 _diffrn_reflns_theta_min 3.23 _diffrn_reflns_theta_full 68.29 _diffrn_measurement_method IP _computing_cell_refinement Scalepack(HKL) _computing_structure_solution 'SIR92 (Altomare et al., 1994)' _atom_sites_solution_primary direct _atom_sites_solution_secondary difmap _exptl_absorpt_correction_type none _exptl_absorpt_correction_T_min ? _exptl_absorpt_correction_T_max ? loop_ _atom_type_symbol _atom_type_description _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source C C 0.0181 0.0091 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' N N 0.0311 0.0180 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' O O 0.0492 0.0322 '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' _exptl_absorpt_coefficient_mu 0.869 _reflns_number_total 1046 _reflns_number_gt 675 _reflns_threshold_expression >2sigma(I) _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _refine_special_details ; Refinement of F^2^ against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F^2^, conventional R-factors R are based on F, with F set to zero for negative F^2^. The threshold expression of F^2^ > 2sigma(F^2^) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F^2^ are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger. ; _refine_ls_structure_factor_coef Fsqd _refine_ls_matrix_type full _refine_ls_weighting_scheme 'calc w=1/[\s^2^(Fo^2^)+ (0.1000P)^2^+0.0000P] where P=(Fo^2^+2Fc^2^)/3' _refine_ls_extinction_method none _refine_ls_extinction_coef ? _refine_ls_number_reflns 1046 _refine_ls_number_parameters 172 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.1113 _refine_ls_R_factor_gt 0.0740 _refine_ls_wR_factor_ref 0.2169 _refine_ls_wR_factor_gt 0.1934 _refine_ls_goodness_of_fit_ref 1.478 _refine_ls_restrained_S_all 1.478 _refine_ls_shift/su_max 0.224 _refine_ls_shift/su_mean 0.033 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_calc_flag _atom_site_refinement_flags _atom_site_disorder_assembly _atom_site_disorder_group O1 O 0.2826(4) 0.0695(9) 0.6588(3) 0.0745(15) Uani 1 d . . . O2 O -0.0340(4) -0.1907(8) 0.2945(3) 0.0610(13) Uani 1 d . . . O3 O -0.0775(4) -0.4546(8) 0.3722(3) 0.0632(14) Uani 1 d . . . N1 N 0.1628(5) 0.1677(10) 0.4179(4) 0.0552(16) Uani 1 d . . . C1 C 0.2565(6) 0.3521(12) 0.4647(4) 0.0518(17) Uani 1 d . . . C2 C 0.3201(6) 0.3465(11) 0.5654(4) 0.0530(17) Uani 1 d . . . C3 C 0.4177(7) 0.5140(14) 0.6287(6) 0.068(2) Uani 1 d . . . C4 C 0.4501(8) 0.6857(16) 0.5891(6) 0.075(2) Uani 1 d . . . C5 C 0.3898(8) 0.6880(15) 0.4902(6) 0.073(2) Uani 1 d . . . C6 C 0.2915(7) 0.5221(12) 0.4251(5) 0.0597(19) Uani 1 d . . . C7 C 0.2596(6) 0.1440(12) 0.5823(4) 0.0588(18) Uani 1 d . . . C8 C 0.1582(6) 0.0355(11) 0.4825(4) 0.0480(16) Uani 1 d . . . C9 C 0.0818(7) -0.1596(13) 0.4655(5) 0.0572(19) Uani 1 d . . . C10 C -0.0141(6) -0.2620(12) 0.3684(4) 0.0545(17) Uani 1 d . . . C11 C -0.1773(9) -0.569(2) 0.2790(6) 0.077(2) Uani 1 d . . . H3 H 0.472(6) 0.486(12) 0.701(5) 0.08(2) Uiso 1 d . . . H4 H 0.524(7) 0.797(14) 0.634(5) 0.09(2) Uiso 1 d . . . H5 H 0.405(5) 0.806(10) 0.460(4) 0.042(17) Uiso 1 d . . . H6 H 0.250(6) 0.526(11) 0.354(5) 0.070(19) Uiso 1 d . . . H1 H 0.119(5) 0.129(9) 0.360(4) 0.038(16) Uiso 1 d . . . H9 H 0.095(5) -0.214(10) 0.519(4) 0.046(16) Uiso 1 d . . . H11A H -0.232(5) -0.674(11) 0.287(4) 0.048(17) Uiso 1 d . . . H11B H -0.131(7) -0.627(13) 0.256(5) 0.10(3) Uiso 1 d . . . H11C H -0.257(7) -0.447(13) 0.238(5) 0.08(2) Uiso 1 d . . . loop_ _atom_site_aniso_label _atom_site_aniso_U_11 _atom_site_aniso_U_22 _atom_site_aniso_U_33 _atom_site_aniso_U_23 _atom_site_aniso_U_13 _atom_site_aniso_U_12 O1 0.079(3) 0.087(4) 0.044(3) 0.002(2) 0.031(3) -0.004(3) O2 0.068(3) 0.065(3) 0.044(3) -0.001(2) 0.031(2) -0.008(2) O3 0.073(3) 0.058(3) 0.052(3) -0.003(2) 0.035(2) -0.013(2) N1 0.058(4) 0.064(4) 0.033(3) -0.005(3) 0.023(3) -0.010(3) C1 0.051(4) 0.059(4) 0.048(4) 0.004(3) 0.032(3) 0.010(4) C2 0.055(4) 0.046(4) 0.058(4) -0.005(3) 0.035(3) 0.000(3) C3 0.054(4) 0.068(5) 0.063(5) -0.010(4) 0.026(4) -0.003(4) C4 0.064(5) 0.072(5) 0.080(6) -0.007(5) 0.040(5) -0.010(4) C5 0.081(6) 0.065(5) 0.077(5) 0.002(5) 0.050(5) -0.009(4) C6 0.065(5) 0.056(4) 0.056(4) -0.003(4) 0.036(4) -0.001(4) C7 0.056(4) 0.061(4) 0.036(3) -0.003(3) 0.016(3) 0.012(4) C8 0.057(4) 0.046(4) 0.049(4) 0.001(3) 0.036(3) 0.006(4) C9 0.065(5) 0.063(5) 0.043(4) 0.011(4) 0.032(4) 0.013(4) C10 0.068(4) 0.044(4) 0.051(4) 0.002(3) 0.036(4) 0.011(4) C11 0.068(6) 0.092(6) 0.064(5) -0.015(5) 0.037(5) -0.029(6) _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 1.228(7) . ? O2 C10 1.200(6) . ? O3 C10 1.348(7) . ? O3 C11 1.452(8) . ? N1 C8 1.352(7) . ? N1 C1 1.385(8) . ? C1 C6 1.373(9) . ? C1 C2 1.397(8) . ? C2 C3 1.387(9) . ? C2 C7 1.471(9) . ? C3 C4 1.357(10) . ? C4 C5 1.377(10) . ? C5 C6 1.393(9) . ? C7 C8 1.510(8) . ? C8 C9 1.346(9) . ? C9 C10 1.455(9) . ? N1 H1 0.82(5) . ? C3 H3 1.00(6) . ? C4 H4 0.99(8) . ? C5 H5 0.91(5) . ? C6 H6 1.00(6) . ? C9 H9 0.88(5) . ? C11 H11A 0.98(5) . ? C11 H11B 0.95(7) . ? C11 H11C 1.06(8) . ? 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 C10 O3 C11 115.6(5) . . ? C8 N1 C1 111.0(5) . . ? C6 C1 N1 128.6(6) . . ? C6 C1 C2 120.6(6) . . ? N1 C1 C2 110.8(6) . . ? C3 C2 C1 122.0(7) . . ? C3 C2 C7 131.7(6) . . ? C1 C2 C7 106.2(6) . . ? C2 C3 C4 117.3(8) . . ? C3 C4 C5 120.8(8) . . ? C4 C5 C6 123.0(8) . . ? C1 C6 C5 116.2(7) . . ? O1 C7 C2 130.0(6) . . ? O1 C7 C8 124.9(6) . . ? C2 C7 C8 105.0(5) . . ? C9 C8 N1 128.6(6) . . ? C9 C8 C7 124.4(6) . . ? N1 C8 C7 107.0(6) . . ? C8 C9 C10 123.1(6) . . ? O2 C10 O3 123.6(6) . . ? O2 C10 C9 125.6(7) . . ? O3 C10 C9 110.8(6) . . ? C8 N1 H1 122(4) . . ? C1 N1 H1 127(4) . . ? C2 C3 H3 120(4) . . ? C4 C3 H3 122(4) . . ? C3 C4 H4 118(4) . . ? C5 C4 H4 121(4) . . ? C4 C5 H5 124(3) . . ? C6 C5 H5 113(3) . . ? C1 C6 H6 123(3) . . ? C5 C6 H6 121(4) . . ? C8 C9 H9 113(4) . . ? C10 C9 H9 124(4) . . ? O3 C11 H11A 109(3) . . ? O3 C11 H11B 103(4) . . ? H11A C11 H11B 125(6) . . ? O3 C11 H11C 110(4) . . ? H11A C11 H11C 86(5) . . ? H11B C11 H11C 123(6) . . ? _diffrn_measured_fraction_theta_max 0.534 _diffrn_measured_fraction_theta_full 0.534 _refine_diff_density_max 0.267 _refine_diff_density_min -0.278 _refine_diff_density_rms 0.070 _publ_section_references ; Mackay, S., Gilmore, C. J.,Edwards, C., Stewart, N. & Shankland, K. (1999). maXus Computer Program for the Solution and Refinement of Crystal Structures. Bruker Nonius, The Netherlands, MacScience, Japan & The University of Glasgow. Johnson, C. K. (1976). ORTEP-II. A Fortran Thermal-Ellipsoid Plot Program. Report ORNL-5138. Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA. Altomare, A., Cascarano, G., Giacovazzo, C., Guagliardi, A., Burla, M. C., Polidori, G. & Camalli, M. (1994). J. Appl. Cryst. 27, 435. Sheldrick, G. M. (1997). SHELXL97. Program for the Refinement of Crystal Structures. University of G\"ottingen, Germany. ;