Supplementary Material (ESI) for Dalton Transactions This journal is (c) The Royal Society of Chemistry 2007 data_global _journal_name_full 'Dalton Trans.' _journal_coden_Cambridge 0222 _publ_contact_author_name 'Partha Mukherjee' _publ_contact_author_address ; Inorganic and Physical Chemistry Indian Institute of Science Bangalore 560012 INDIA ; _publ_contact_author_email PSM@IPC.IISC.ERNET.IN _publ_section_title ; Dual role of azide in the formation of a 3D coordination polymer containing bridging 5-pyrimidinecarboxylate ; loop_ _publ_author_name 'Partha Mukherjee' 'Rajesh Chakraborty' 'Oindrila Sengupta' # Attachment 'final-cif.cif' data_os15lt_m _database_code_depnum_ccdc_archive 'CCDC 655473' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'C5 H3 Mn N5 O2.25' _chemical_formula_sum 'C5 H3 Mn N5 O2.25' _chemical_formula_weight 224.06 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' Mn Mn 0.3368 0.7283 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting Tetragonal _symmetry_space_group_name_H-M P4(2)/nmc _symmetry_space_group_name_Hall 'P 4ac 2a' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x+1/2, -y+1/2, z' '-y+1/2, x, z+1/2' 'y, -x+1/2, z+1/2' '-x, y+1/2, -z' 'x+1/2, -y, -z' 'y+1/2, x+1/2, -z+1/2' '-y, -x, -z+1/2' '-x, -y, -z' 'x-1/2, y-1/2, -z' 'y-1/2, -x, -z-1/2' '-y, x-1/2, -z-1/2' 'x, -y-1/2, z' '-x-1/2, y, z' '-y-1/2, -x-1/2, z-1/2' 'y, x, z-1/2' _cell_length_a 10.4583(3) _cell_length_b 10.4583(3) _cell_length_c 13.6296(8) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 1490.75(11) _cell_formula_units_Z 8 _cell_measurement_temperature 293(2) _cell_measurement_reflns_used 3967 _cell_measurement_theta_min 2.5 _cell_measurement_theta_max 28.0 _exptl_crystal_description 'rectangular block' _exptl_crystal_colour yellow _exptl_crystal_size_max 0.12 _exptl_crystal_size_mid 0.10 _exptl_crystal_size_min 0.08 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 1.997 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 888 _exptl_absorpt_coefficient_mu 1.744 _exptl_absorpt_correction_type empirical _exptl_absorpt_correction_T_min 0.8180 _exptl_absorpt_correction_T_max 0.8731 _exptl_absorpt_process_details SADABS _exptl_special_details ; 'none' ; _diffrn_ambient_temperature 293(2) _diffrn_radiation_wavelength 0.71073 _diffrn_radiation_type MoK\a _diffrn_radiation_source 'fine-focus sealed tube' _diffrn_radiation_monochromator graphite _diffrn_measurement_device_type 'CCD area detector' _diffrn_measurement_method 'phi and omega scans' _diffrn_detector_area_resol_mean ? _diffrn_standards_number ? _diffrn_standards_interval_count ? _diffrn_standards_interval_time ? _diffrn_standards_decay_% ? _diffrn_reflns_number 12245 _diffrn_reflns_av_R_equivalents 0.0252 _diffrn_reflns_av_sigmaI/netI 0.0117 _diffrn_reflns_limit_h_min -13 _diffrn_reflns_limit_h_max 13 _diffrn_reflns_limit_k_min -13 _diffrn_reflns_limit_k_max 13 _diffrn_reflns_limit_l_min -17 _diffrn_reflns_limit_l_max 17 _diffrn_reflns_theta_min 2.45 _diffrn_reflns_theta_max 28.02 _reflns_number_total 1001 _reflns_number_gt 832 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'Bruker SMART' _computing_cell_refinement 'Bruker SMART' _computing_data_reduction 'Bruker SAINT' _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics 'WINGX for Windows(Farrugia, 1997)' _computing_publication_material 'CIFTAB in SHELXL97 (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 _refine_ls_weighting_details 'calc w=1/[\s^2^(Fo^2^)+(0.0431P)^2^+1.5421P] 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 1001 _refine_ls_number_parameters 73 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0342 _refine_ls_R_factor_gt 0.0273 _refine_ls_wR_factor_ref 0.0802 _refine_ls_wR_factor_gt 0.0756 _refine_ls_goodness_of_fit_ref 1.048 _refine_ls_restrained_S_all 1.048 _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_symmetry_multiplicity _atom_site_calc_flag _atom_site_refinement_flags _atom_site_disorder_assembly _atom_site_disorder_group Mn1 Mn 0.43282(2) 0.56718(2) 0.2500 0.01328(15) Uani 1 2 d S . . O1 O 0.35735(12) 0.47351(13) 0.12126(9) 0.0182(3) Uani 1 1 d . . . N1 N 0.4168(2) 0.7500 0.17067(16) 0.0232(5) Uani 1 2 d S . . N2 N 0.4148(3) 0.7500 0.08090(19) 0.0346(7) Uani 1 2 d S . . N3 N 0.4119(4) 0.7500 -0.0056(2) 0.0557(11) Uani 1 2 d S . . N4 N 0.63634(15) 0.54746(16) 0.18210(11) 0.0198(3) Uani 1 1 d . . . C1 C 0.63823(18) 0.54543(19) 0.08350(13) 0.0201(4) Uani 1 1 d . . . H1 H 0.5608 0.5452 0.0499 0.024 Uiso 1 1 calc R . . C2 C 0.7500 0.5437(2) 0.03010(17) 0.0154(5) Uani 1 2 d S . . C3 C 0.7500 0.5480(3) 0.22745(19) 0.0194(5) Uani 1 2 d S . . H3 H 0.7500 0.5488 0.2957 0.023 Uiso 1 2 calc SR . . C4 C 0.2500 0.4686(2) 0.08046(17) 0.0138(5) Uani 1 2 d S . . O1W O 0.2500 0.7500 -1.344(3) 0.34(2) Uani 0.50 4 d SP . . 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 Mn1 0.01581(17) 0.01581(17) 0.0082(2) -0.00051(10) -0.00051(10) -0.00054(13) O1 0.0180(6) 0.0256(7) 0.0110(6) -0.0030(5) -0.0023(5) -0.0003(5) N1 0.0372(14) 0.0168(11) 0.0156(11) 0.000 -0.0064(10) 0.000 N2 0.0587(19) 0.0218(13) 0.0231(13) 0.000 -0.0036(13) 0.000 N3 0.118(3) 0.0271(15) 0.0217(13) 0.000 -0.0030(17) 0.000 N4 0.0185(8) 0.0297(9) 0.0112(7) -0.0044(6) 0.0010(6) -0.0020(7) C1 0.0163(9) 0.0304(10) 0.0136(8) -0.0039(7) -0.0006(7) -0.0012(8) C2 0.0180(12) 0.0176(12) 0.0107(11) -0.0022(9) 0.000 0.000 C3 0.0208(13) 0.0272(14) 0.0103(11) -0.0025(10) 0.000 0.000 C4 0.0165(11) 0.0149(12) 0.0101(11) -0.0019(9) 0.000 0.000 O1W 0.095(16) 0.38(4) 0.53(6) 0.000 0.000 0.000 _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 Mn1 O1 2.1591(12) . ? Mn1 O1 2.1591(12) 8_665 ? Mn1 N1 2.2030(11) . ? Mn1 N1 2.2030(11) 11_566 ? Mn1 N4 2.3300(16) . ? Mn1 N4 2.3300(16) 8_665 ? O1 C4 1.2539(16) . ? N1 N2 1.224(3) . ? N1 Mn1 2.2030(11) 12_666 ? N2 N3 1.179(4) . ? N4 C3 1.3399(19) . ? N4 C1 1.344(2) . ? C1 C2 1.377(2) . ? C2 C1 1.377(2) 14_755 ? C2 C4 1.512(3) 9_665 ? C3 N4 1.3399(19) 14_755 ? C4 O1 1.2539(16) 14_655 ? C4 C2 1.512(3) 9_665 ? 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 O1 Mn1 O1 172.86(7) . 8_665 ? O1 Mn1 N1 88.11(6) . . ? O1 Mn1 N1 96.67(6) 8_665 . ? O1 Mn1 N1 96.67(6) . 11_566 ? O1 Mn1 N1 88.11(6) 8_665 11_566 ? N1 Mn1 N1 96.25(13) . 11_566 ? O1 Mn1 N4 88.34(5) . . ? O1 Mn1 N4 86.60(5) 8_665 . ? N1 Mn1 N4 87.21(8) . . ? N1 Mn1 N4 173.99(6) 11_566 . ? O1 Mn1 N4 86.60(5) . 8_665 ? O1 Mn1 N4 88.34(5) 8_665 8_665 ? N1 Mn1 N4 173.99(6) . 8_665 ? N1 Mn1 N4 87.21(8) 11_566 8_665 ? N4 Mn1 N4 89.78(8) . 8_665 ? C4 O1 Mn1 134.94(13) . . ? N2 N1 Mn1 119.48(5) . 12_666 ? N2 N1 Mn1 119.48(5) . . ? Mn1 N1 Mn1 120.44(10) 12_666 . ? N3 N2 N1 179.5(4) . . ? C3 N4 C1 116.63(17) . . ? C3 N4 Mn1 128.81(13) . . ? C1 N4 Mn1 114.33(13) . . ? N4 C1 C2 122.76(18) . . ? C1 C2 C1 116.2(2) 14_755 . ? C1 C2 C4 121.85(11) 14_755 9_665 ? C1 C2 C4 121.85(11) . 9_665 ? N4 C3 N4 125.0(2) . 14_755 ? O1 C4 O1 127.1(2) 14_655 . ? O1 C4 C2 116.44(11) 14_655 9_665 ? O1 C4 C2 116.44(11) . 9_665 ? _diffrn_measured_fraction_theta_max 0.996 _diffrn_reflns_theta_full 28.02 _diffrn_measured_fraction_theta_full 0.996 _refine_diff_density_max 1.008 _refine_diff_density_min -0.547 _refine_diff_density_rms 0.075