# Supplementary Material (ESI) for Chemical Communications # This journal is (c) The Royal Society of Chemistry 2009 data_global _journal_name_full Chem.Commun. _journal_coden_Cambridge 0182 _publ_contact_author_name 'Len MacGillivray' _publ_contact_author_email LEN-MACGILLIVRAY@UIOWA.EDU _publ_section_title ; ineering cocrystal and polymorph architecture via pseudoseeding ; loop_ _publ_author_name 'Len MacGillivray' 'Tomislav Friscic' # Attachment 'deposit1.cif' data_(RES).(4,4'-BPE) _database_code_depnum_ccdc_archive 'CCDC 707408' _audit_creation_method SHELXL-97 _chemical_name_systematic ; resorcinol . trans-1,2-bis(4-pyridyl)ethylene 1/2 form 2 ; _chemical_name_common 'resorcinol . trans-1,2-bis(4-pyridyl)ethylene 1/2 form 2' _chemical_melting_point ? _chemical_formula_moiety ? _chemical_formula_sum 'C18 H16 N2 O2' _chemical_formula_weight 292.33 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' _symmetry_cell_setting monoclinic _symmetry_space_group_name_H-M P21/n loop_ _symmetry_equiv_pos_as_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 10.1465(10) _cell_length_b 7.1871(7) _cell_length_c 20.042(2) _cell_angle_alpha 90.00 _cell_angle_beta 94.797(5) _cell_angle_gamma 90.00 _cell_volume 1456.4(2) _cell_formula_units_Z 4 _cell_measurement_temperature 190(2) _cell_measurement_reflns_used 5565 _cell_measurement_theta_min 1.00 _cell_measurement_theta_max 27.48 _exptl_crystal_description prism _exptl_crystal_colour colourless _exptl_crystal_size_max 0.19 _exptl_crystal_size_mid 0.14 _exptl_crystal_size_min 0.10 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 1.333 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 616 _exptl_absorpt_coefficient_mu 0.088 _exptl_absorpt_correction_type none _exptl_absorpt_process_details ? _exptl_special_details ; ? ; _diffrn_ambient_temperature 190(2) _diffrn_radiation_wavelength 0.71069 _diffrn_radiation_type MoK\a _diffrn_radiation_source 'fine-focus sealed tube' _diffrn_radiation_monochromator graphite _diffrn_measurement_device_type ? _diffrn_measurement_method ? _diffrn_detector_area_resol_mean ? _diffrn_standards_number ? _diffrn_standards_interval_count ? _diffrn_standards_interval_time ? _diffrn_standards_decay_% ? _diffrn_reflns_number 10675 _diffrn_reflns_av_R_equivalents 0.0419 _diffrn_reflns_av_sigmaI/netI 0.0497 _diffrn_reflns_limit_h_min -13 _diffrn_reflns_limit_h_max 13 _diffrn_reflns_limit_k_min -8 _diffrn_reflns_limit_k_max 9 _diffrn_reflns_limit_l_min -25 _diffrn_reflns_limit_l_max 22 _diffrn_reflns_theta_min 2.04 _diffrn_reflns_theta_max 27.49 _reflns_number_total 3342 _reflns_number_gt 2314 _reflns_threshold_expression >2sigma(I) _computing_data_collection ? _computing_cell_refinement ? _computing_data_reduction ? _computing_structure_solution ? _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics ? _computing_publication_material ? _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 _refine_ls_weighting_details 'calc w=1/[\s^2^(Fo^2^)+(0.0620P)^2^+0.2458P] where P=(Fo^2^+2Fc^2^)/3' _atom_sites_solution_primary direct _atom_sites_solution_secondary difmap _atom_sites_solution_hydrogens geom _refine_ls_hydrogen_treatment constr _refine_ls_extinction_method none _refine_ls_extinction_coef ? _refine_ls_number_reflns 3342 _refine_ls_number_parameters 201 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0756 _refine_ls_R_factor_gt 0.0442 _refine_ls_wR_factor_ref 0.1292 _refine_ls_wR_factor_gt 0.1035 _refine_ls_goodness_of_fit_ref 1.029 _refine_ls_restrained_S_all 1.029 _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_symmetry_multiplicity _atom_site_calc_flag _atom_site_refinement_flags _atom_site_disorder_assembly _atom_site_disorder_group O1 O 0.93157(11) 0.62071(16) 0.55378(5) 0.0367(3) Uani 1 1 d . . . H1 H 1.0081 0.6658 0.5547 0.055 Uiso 1 1 calc R . . O2 O 0.54331(10) 0.64940(17) 0.66535(5) 0.0365(3) Uani 1 1 d . . . H2 H 0.5158 0.6725 0.7029 0.055 Uiso 1 1 calc R . . N1 N 1.17087(13) 0.78252(19) 0.53137(7) 0.0359(4) Uani 1 1 d . . . N2 N 1.90742(13) 0.80203(18) 0.27599(6) 0.0306(3) Uani 1 1 d . . . C1 C 1.15543(16) 0.8645(2) 0.47144(8) 0.0351(4) Uani 1 1 d . . . H1A H 1.0700 0.9093 0.4564 0.042 Uiso 1 1 calc R . . C2 C 1.25633(16) 0.8879(2) 0.42998(8) 0.0322(4) Uani 1 1 d . . . H2A H 1.2393 0.9460 0.3876 0.039 Uiso 1 1 calc R . . C3 C 1.38310(15) 0.8260(2) 0.45078(7) 0.0270(3) Uani 1 1 d . . . C4 C 1.40052(15) 0.7460(2) 0.51444(8) 0.0311(4) Uani 1 1 d . . . H4 H 1.4856 0.7049 0.5318 0.037 Uiso 1 1 calc R . . C5 C 1.29377(16) 0.7271(2) 0.55186(8) 0.0340(4) Uani 1 1 d . . . H5 H 1.3080 0.6713 0.5948 0.041 Uiso 1 1 calc R . . C6 C 1.48813(15) 0.8438(2) 0.40523(8) 0.0304(4) Uani 1 1 d . . . H6 H 1.4646 0.9011 0.3632 0.036 Uiso 1 1 calc R . . C7 C 1.61244(16) 0.7883(2) 0.41650(8) 0.0301(4) Uani 1 1 d . . . H7 H 1.6383 0.7370 0.4593 0.036 Uiso 1 1 calc R . . C8 C 1.71357(15) 0.7994(2) 0.36855(7) 0.0272(3) Uani 1 1 d . . . C9 C 1.69199(16) 0.8870(2) 0.30627(8) 0.0330(4) Uani 1 1 d . . . H9 H 1.6104 0.9478 0.2941 0.040 Uiso 1 1 calc R . . C10 C 1.78984(16) 0.8842(2) 0.26286(8) 0.0336(4) Uani 1 1 d . . . H10 H 1.7729 0.9445 0.2208 0.040 Uiso 1 1 calc R . . C11 C 1.83691(15) 0.7178(2) 0.38301(8) 0.0302(4) Uani 1 1 d . . . H11 H 1.8578 0.6597 0.4251 0.036 Uiso 1 1 calc R . . C12 C 1.92905(15) 0.7214(2) 0.33612(8) 0.0307(4) Uani 1 1 d . . . H12 H 2.0122 0.6636 0.3471 0.037 Uiso 1 1 calc R . . C13 C 0.87414(15) 0.6729(2) 0.61015(7) 0.0268(3) Uani 1 1 d . . . C14 C 0.74121(14) 0.6320(2) 0.61256(7) 0.0268(3) Uani 1 1 d . . . H14 H 0.6950 0.5669 0.5766 0.032 Uiso 1 1 calc R . . C15 C 0.67528(15) 0.6861(2) 0.66745(7) 0.0271(4) Uani 1 1 d . . . C16 C 0.74410(16) 0.7756(2) 0.72111(8) 0.0321(4) Uani 1 1 d . . . H16 H 0.7001 0.8120 0.7590 0.039 Uiso 1 1 calc R . . C17 C 0.87771(16) 0.8109(2) 0.71850(8) 0.0344(4) Uani 1 1 d . . . H17 H 0.9252 0.8701 0.7555 0.041 Uiso 1 1 calc R . . C18 C 0.94389(15) 0.7623(2) 0.66353(8) 0.0318(4) Uani 1 1 d . . . H18 H 1.0353 0.7895 0.6623 0.038 Uiso 1 1 calc R . . 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 0.0274(6) 0.0507(7) 0.0334(6) -0.0062(5) 0.0111(5) -0.0017(5) O2 0.0249(6) 0.0555(7) 0.0305(6) 0.0003(6) 0.0099(5) -0.0033(5) N1 0.0299(8) 0.0451(8) 0.0339(8) -0.0045(7) 0.0099(6) -0.0044(6) N2 0.0276(7) 0.0337(7) 0.0316(7) -0.0013(6) 0.0084(6) -0.0014(6) C1 0.0253(9) 0.0423(9) 0.0386(9) -0.0008(8) 0.0069(7) 0.0029(7) C2 0.0321(9) 0.0336(9) 0.0315(8) 0.0022(7) 0.0067(7) 0.0016(7) C3 0.0267(8) 0.0264(7) 0.0287(8) -0.0035(6) 0.0067(6) -0.0017(6) C4 0.0264(8) 0.0377(9) 0.0295(8) -0.0003(7) 0.0043(7) -0.0004(7) C5 0.0326(9) 0.0428(9) 0.0277(8) 0.0008(7) 0.0084(7) -0.0050(7) C6 0.0297(9) 0.0353(8) 0.0272(8) 0.0023(7) 0.0081(6) 0.0006(7) C7 0.0320(9) 0.0331(8) 0.0263(8) 0.0022(7) 0.0088(7) 0.0005(7) C8 0.0265(8) 0.0287(8) 0.0271(8) -0.0017(6) 0.0067(6) -0.0012(6) C9 0.0274(9) 0.0390(9) 0.0334(9) 0.0071(7) 0.0081(7) 0.0062(7) C10 0.0335(9) 0.0397(9) 0.0286(8) 0.0068(7) 0.0089(7) 0.0027(7) C11 0.0280(9) 0.0359(9) 0.0269(8) 0.0025(7) 0.0024(7) 0.0006(7) C12 0.0228(8) 0.0354(9) 0.0342(9) -0.0001(7) 0.0041(7) 0.0014(6) C13 0.0252(8) 0.0291(8) 0.0270(8) 0.0021(6) 0.0068(6) 0.0028(6) C14 0.0256(8) 0.0299(8) 0.0249(8) 0.0004(6) 0.0027(6) -0.0008(6) C15 0.0231(8) 0.0306(8) 0.0283(8) 0.0050(7) 0.0068(6) -0.0001(6) C16 0.0348(9) 0.0360(9) 0.0267(8) -0.0020(7) 0.0094(7) -0.0011(7) C17 0.0341(9) 0.0387(9) 0.0301(9) -0.0046(7) 0.0007(7) -0.0041(7) C18 0.0227(8) 0.0365(9) 0.0365(9) -0.0011(7) 0.0042(7) -0.0022(7) _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 C13 1.3662(18) . ? O2 C15 1.3620(17) . ? N1 C1 1.335(2) . ? N1 C5 1.340(2) . ? N2 C10 1.337(2) . ? N2 C12 1.339(2) . ? C1 C2 1.382(2) . ? C2 C3 1.392(2) . ? C3 C4 1.397(2) . ? C3 C6 1.466(2) . ? C4 C5 1.375(2) . ? C6 C7 1.324(2) . ? C7 C8 1.466(2) . ? C8 C11 1.390(2) . ? C8 C9 1.399(2) . ? C9 C10 1.374(2) . ? C11 C12 1.380(2) . ? C13 C14 1.385(2) . ? C13 C18 1.390(2) . ? C14 C15 1.390(2) . ? C15 C16 1.390(2) . ? C16 C17 1.384(2) . ? C17 C18 1.382(2) . ? 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 C1 N1 C5 116.29(14) . . ? C10 N2 C12 116.40(13) . . ? N1 C1 C2 123.89(15) . . ? C1 C2 C3 119.58(15) . . ? C2 C3 C4 116.64(14) . . ? C2 C3 C6 119.18(14) . . ? C4 C3 C6 124.17(14) . . ? C5 C4 C3 119.57(15) . . ? N1 C5 C4 123.97(15) . . ? C7 C6 C3 126.83(15) . . ? C6 C7 C8 125.52(15) . . ? C11 C8 C9 116.53(14) . . ? C11 C8 C7 120.52(14) . . ? C9 C8 C7 122.94(14) . . ? C10 C9 C8 119.42(15) . . ? N2 C10 C9 124.17(15) . . ? C12 C11 C8 119.96(14) . . ? N2 C12 C11 123.48(14) . . ? O1 C13 C14 117.04(13) . . ? O1 C13 C18 122.58(14) . . ? C14 C13 C18 120.38(14) . . ? C13 C14 C15 120.19(14) . . ? O2 C15 C14 117.28(13) . . ? O2 C15 C16 122.85(14) . . ? C14 C15 C16 119.86(14) . . ? C17 C16 C15 119.05(15) . . ? C18 C17 C16 121.76(15) . . ? C17 C18 C13 118.71(15) . . ? 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 C5 N1 C1 C2 2.3(2) . . . . ? N1 C1 C2 C3 -0.8(2) . . . . ? C1 C2 C3 C4 -1.4(2) . . . . ? C1 C2 C3 C6 177.24(14) . . . . ? C2 C3 C4 C5 2.0(2) . . . . ? C6 C3 C4 C5 -176.57(15) . . . . ? C1 N1 C5 C4 -1.6(2) . . . . ? C3 C4 C5 N1 -0.5(3) . . . . ? C2 C3 C6 C7 -178.33(15) . . . . ? C4 C3 C6 C7 0.2(3) . . . . ? C3 C6 C7 C8 176.64(14) . . . . ? C6 C7 C8 C11 -172.69(16) . . . . ? C6 C7 C8 C9 6.0(3) . . . . ? C11 C8 C9 C10 1.6(2) . . . . ? C7 C8 C9 C10 -177.09(15) . . . . ? C12 N2 C10 C9 -1.2(2) . . . . ? C8 C9 C10 N2 -0.1(3) . . . . ? C9 C8 C11 C12 -1.9(2) . . . . ? C7 C8 C11 C12 176.86(14) . . . . ? C10 N2 C12 C11 0.9(2) . . . . ? C8 C11 C12 N2 0.6(2) . . . . ? O1 C13 C14 C15 -178.00(13) . . . . ? C18 C13 C14 C15 2.3(2) . . . . ? C13 C14 C15 O2 177.04(13) . . . . ? C13 C14 C15 C16 -2.3(2) . . . . ? O2 C15 C16 C17 -178.68(14) . . . . ? C14 C15 C16 C17 0.6(2) . . . . ? C15 C16 C17 C18 1.1(2) . . . . ? C16 C17 C18 C13 -1.1(2) . . . . ? O1 C13 C18 C17 179.70(14) . . . . ? C14 C13 C18 C17 -0.6(2) . . . . ? _diffrn_measured_fraction_theta_max 0.999 _diffrn_reflns_theta_full 27.49 _diffrn_measured_fraction_theta_full 0.999 _refine_diff_density_max 0.231 _refine_diff_density_min -0.220 _refine_diff_density_rms 0.052