# Electronic Supplementary Material (ESI) for CrystEngComm # This journal is © The Royal Society of Chemistry 2012 data_global _journal_name_full CrystEngComm _journal_coden_cambridge 1350 _journal_year ? _journal_volume ? _journal_page_first ? _publ_contact_author_name 'Karla Fejfarova' _publ_contact_author_email fejfarov@fzu.cz loop_ _publ_author_name 'I. Matulkova' 'J. Cihelka' 'M. Pojarova' 'K. Fejfarova' 'M. Dusek' 'P. Vanek' ; J.Kroupa ; 'R. Krupkova' 'J. Fabry' 'I. Nemec' data_I _database_code_depnum_ccdc_archive 'CCDC 831896' #TrackingRef '6000_web_deposit_cif_file_0_KarlaFejfarova_1309265877.dat_h2seo4_1_precislovany.cif' #======================================================================= # 5. CHEMICAL DATA _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_formula_moiety '2(C2 H6 N5), O4 Se, 2(H2 O)' _chemical_formula_structural ? _chemical_formula_analytical ? _chemical_formula_iupac ? _chemical_formula_sum 'C4 H16 N10 O6 Se1' _chemical_formula_weight 379.2 _chemical_melting_point ? _chemical_compound_source ? _chemical_absolute_configuration . #======================================================================= # 6. CRYSTAL DATA _symmetry_cell_setting triclinic _symmetry_space_group_name_H-M 'P -1' _symmetry_space_group_name_Hall '-P 1' _symmetry_Int_Tables_number 2 loop_ _symmetry_equiv_pos_site_id _symmetry_equiv_pos_as_xyz 1 x,y,z 2 -x,-y,-z _cell_length_a 6.16030(10) _cell_length_b 6.3726(2) _cell_length_c 17.9756(5) _cell_angle_alpha 97.743(2) _cell_angle_beta 99.269(2) _cell_angle_gamma 96.969(2) _cell_volume 682.69(3) _cell_formula_units_Z 2 _cell_measurement_reflns_used 10452 _cell_measurement_theta_min 5.0438 _cell_measurement_theta_max 66.8427 _cell_measurement_temperature 120 _cell_special_details ; ? ; _exptl_crystal_density_diffrn 1.8441 _exptl_crystal_density_meas ? _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 384 _exptl_absorpt_coefficient_mu 4.226 _exptl_crystal_description prism _exptl_crystal_size_max 0.1995 _exptl_crystal_size_mid 0.1537 _exptl_crystal_size_min 0.1139 _exptl_crystal_colour colorless _exptl_absorpt_correction_T_min 0.575 _exptl_absorpt_correction_T_max 0.724 _exptl_absorpt_correction_type analytical _exptl_absorpt_process_details ; CrysAlisPro, Oxford Diffraction (2009) Analytical numeric absorption correction using a multifaceted crystal model. ; #======================================================================= # 7. EXPERIMENTAL DATA _exptl_special_details ? _diffrn_ambient_temperature 120 _diffrn_radiation_type 'Cu K\a' _diffrn_radiation_source 'X-ray tube' _diffrn_radiation_wavelength 1.54184 _diffrn_measurement_device 'four-cycle diffractometer' _diffrn_radiation_monochromator mirror _diffrn_measurement_device_type 'Goniometer Xcalibur, detector: Atlas (Gemini ultra Cu)' _diffrn_detector_area_resol_mean 10.3784 _diffrn_measurement_method 'Rotation method data acquisition using \w scans' _diffrn_reflns_number 10277 _diffrn_reflns_theta_min 5.05 _diffrn_reflns_theta_max 66.99 _diffrn_reflns_theta_full 66.38 _diffrn_measured_fraction_theta_max 0.97 _diffrn_measured_fraction_theta_full 0.98 _diffrn_reflns_av_R_equivalents 0.0219 _diffrn_reflns_av_sigmaI/netI 0.0042 _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 -20 _diffrn_reflns_limit_l_max 21 _diffrn_reflns_reduction_process ; Integration of the CCD images was done by program Crysalis RED (Oxford diffraction, 2009). The same program was used for indexing of the crystal shape and absorption correction. ; #======================================================================= # 8. REFINEMENT DATA _refine_special_details ; The refinement was carried out against all reflections. The conventional R-factor is always based on F. The goodness of fit as well as the weighted R-factor are based on F and F^2^ for refinement carried out on F and F^2^, respectively. The threshold expression is used only for calculating R-factors etc. and it is not relevant to the choice of reflections for refinement. The program used for refinement, Jana2006, uses the weighting scheme based on the experimental expectations, see _refine_ls_weighting_details, that does not force S to be one. Therefore the values of S are usually larger than the ones from the SHELX program. ; _reflns_number_total 2365 _reflns_number_gt 2342 _reflns_threshold_expression I>3\s(I) _refine_ls_structure_factor_coef Fsqd _refine_ls_R_factor_gt 0.0221 _refine_ls_wR_factor_gt 0.0763 _refine_ls_R_factor_all 0.0223 _refine_ls_wR_factor_ref 0.0765 _refine_ls_goodness_of_fit_ref 1.86 _refine_ls_goodness_of_fit_gt 1.87 _refine_ls_restrained_S_gt ? _refine_ls_restrained_S_all ? _refine_ls_number_reflns 2365 _refine_ls_number_parameters 239 _refine_ls_number_restraints 16 _refine_ls_number_constraints 16 _refine_ls_weighting_scheme sigma _refine_ls_weighting_details w=1/(\s^2^(I)+0.0016I^2^) _refine_ls_hydrogen_treatment refxyz _refine_ls_shift/su_max 0.0072 _refine_ls_shift/su_mean 0.0005 _refine_diff_density_max 0.31 _refine_diff_density_min -0.32 _refine_ls_extinction_method 'B-C type 1 Lorentzian isotropic (Becker & Coppens, 1974)' _refine_ls_extinction_coef 290(90) _refine_ls_abs_structure_details ? _refine_ls_abs_structure_Flack ? _refine_ls_abs_structure_Rogers ? loop_ _atom_type_symbol _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source C 0.0181 0.0091 'International Tables Vol C tables 4.2.6.8 and 6.1.1.1' H 0.0000 0.0000 'International Tables Vol C tables 4.2.6.8 and 6.1.1.1' N 0.0311 0.0180 'International Tables Vol C tables 4.2.6.8 and 6.1.1.1' O 0.0492 0.0322 'International Tables Vol C tables 4.2.6.8 and 6.1.1.1' Se -0.7943 1.1372 'International Tables Vol C tables 4.2.6.8 and 6.1.1.1' _computing_data_collection 'Crysalis CCD (Oxford diffraction, 2009)' _computing_cell_refinement 'Crysalis RED (Oxford diffraction, 2009)' _computing_data_reduction 'Crysalis RED' _computing_structure_solution 'SIR2002 (Burla et al., 2003)' _computing_structure_refinement "Jana2006 (Pet\3\s(I) _refine_ls_structure_factor_coef Fsqd _refine_ls_R_factor_gt 0.0270 _refine_ls_wR_factor_gt 0.0824 _refine_ls_R_factor_all 0.0315 _refine_ls_wR_factor_ref 0.0848 _refine_ls_goodness_of_fit_ref 1.74 _refine_ls_goodness_of_fit_gt 1.80 _refine_ls_restrained_S_gt ? _refine_ls_restrained_S_all ? _refine_ls_number_reflns 2042 _refine_ls_number_parameters 238 _refine_ls_number_restraints 0 _refine_ls_number_constraints 16 _refine_ls_weighting_scheme sigma _refine_ls_weighting_details w=1/(\s^2^(I)+0.0016I^2^) _refine_ls_hydrogen_treatment refxyz _refine_ls_shift/su_max 0.0089 _refine_ls_shift/su_mean 0.0008 _refine_diff_density_max 0.22 _refine_diff_density_min -0.27 _refine_ls_extinction_method none _refine_ls_extinction_coef ? _refine_ls_abs_structure_details ? _refine_ls_abs_structure_Flack ? _refine_ls_abs_structure_Rogers ? loop_ _atom_type_symbol _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source C 0.018 0.009 'International Tables Vol C tables 4.2.6.8 and 6.1.1.1' H 0.000 0.000 'International Tables Vol C tables 4.2.6.8 and 6.1.1.1' N 0.031 0.018 'International Tables Vol C tables 4.2.6.8 and 6.1.1.1' O 0.049 0.032 'International Tables Vol C tables 4.2.6.8 and 6.1.1.1' S 0.333 0.557 'International Tables Vol C tables 4.2.6.8 and 6.1.1.1' _computing_data_collection 'Crysalis CCD (Oxford diffraction, 2009)' _computing_cell_refinement 'Crysalis RED (Oxford diffraction, 2009)' _computing_data_reduction 'Crysalis RED' _computing_structure_solution 'SIR2002 (Burla et al., 2003)' _computing_structure_refinement "Jana2006 (Pet\2sigma(I) _computing_data_collection 'Crysalis CCD (Oxford Diffraction, 2007)' _computing_cell_refinement 'Crysalis RED (Oxford Diffraction, 2007)' _computing_data_reduction 'Crysalis RED (Oxford Diffraction, 2007)' _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics ? _computing_publication_material 'publCIF (MacMahon, 2008)' _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. Hydrogen atoms were located from the maps of electron density and left unrestrained. ; _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^)+(0.0503P)^2^+0.6633P] 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 1907 _refine_ls_number_parameters 154 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0298 _refine_ls_R_factor_gt 0.0290 _refine_ls_wR_factor_ref 0.0771 _refine_ls_wR_factor_gt 0.0764 _refine_ls_goodness_of_fit_ref 1.038 _refine_ls_restrained_S_all 1.038 _refine_ls_shift/su_max 0.002 _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 O1W O 0.80397(18) 0.37926(4) 0.84901(14) 0.0171(3) Uani 1 1 d . . . H1W H 0.7733 0.3680 0.7663 0.019 Uiso 1 1 d . . . H2W H 0.6817 0.3876 0.8766 0.034 Uiso 1 1 d . . . Cl1 Cl 0.23710(6) 0.662406(15) 0.51395(5) 0.01539(15) Uani 1 1 d . . . Cl2 Cl 0.15283(6) 0.902642(15) 0.50311(5) 0.01811(15) Uani 1 1 d . . . C10 C 0.6642(3) 0.73486(6) 0.30720(19) 0.0134(4) Uani 1 1 d . . . C12 C 0.3837(3) 0.79050(6) 0.28188(19) 0.0134(3) Uani 1 1 d . . . N11 N 0.4687(2) 0.74511(5) 0.21884(16) 0.0125(3) Uani 1 1 d . . . H11A H 0.4206 0.7309 0.1393 0.013 Uiso 1 1 d . . . N9 N 0.7029(2) 0.77098(6) 0.42381(17) 0.0147(3) Uani 1 1 d . . . H8A H 0.5132 0.8317 0.4638 0.014 Uiso 1 1 d . . . N8 N 0.5220(2) 0.80602(5) 0.40393(16) 0.0147(3) Uani 1 1 d . . . N14 N 0.7963(2) 0.69324(6) 0.27497(18) 0.0229(4) Uani 1 1 d . . . H14A H 0.7502 0.6684 0.2077 0.025 Uiso 1 1 d . . . H14B H 0.9042 0.6874 0.3409 0.023 Uiso 1 1 d . . . N13 N 0.1989(2) 0.81509(6) 0.22553(18) 0.0202(3) Uani 1 1 d . . . H13A H 0.1085 0.7966 0.1616 0.031 Uiso 1 1 d . . . H13B H 0.1525 0.8389 0.2844 0.025 Uiso 1 1 d . . . C3 C 0.7846(3) 0.54442(6) 0.5864(2) 0.0141(4) Uani 1 1 d . . . C5 C 1.0684(3) 0.52223(6) 0.75227(19) 0.0145(4) Uani 1 1 d . . . N4 N 0.9851(2) 0.56281(5) 0.65596(16) 0.0150(3) Uani 1 1 d . . . H4A H 1.0575 0.5915 0.6226 0.027 Uiso 1 1 d . . . N1 N 0.9224(2) 0.48247(5) 0.74134(17) 0.0161(3) Uani 1 1 d . . . H1A H 0.9278 0.4542 0.7899 0.028 Uiso 1 1 d . . . N2 N 0.7390(2) 0.49596(6) 0.63671(17) 0.0162(3) Uani 1 1 d . . . N6 N 1.2579(2) 0.52232(6) 0.84162(19) 0.0225(4) Uani 1 1 d . . . H6A H 1.3485 0.5496 0.8453 0.034 Uiso 1 1 d . . . H6B H 1.3006 0.4928 0.8823 0.029 Uiso 1 1 d . . . N7 N 0.6627(2) 0.57376(6) 0.47266(18) 0.0202(3) Uani 1 1 d . . . H7B H 0.5396 0.5578 0.4471 0.029 Uiso 1 1 d . . . H7A H 0.6572 0.6077 0.4885 0.029 Uiso 1 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 O1W 0.0180(6) 0.0158(6) 0.0169(6) -0.0002(5) -0.0029(5) 0.0004(5) Cl1 0.0143(2) 0.0137(2) 0.0176(2) 0.00018(14) -0.00285(16) -0.00019(14) Cl2 0.0182(3) 0.0158(2) 0.0199(2) 0.00037(15) -0.00227(17) 0.00356(15) C10 0.0143(8) 0.0120(8) 0.0135(8) 0.0016(7) -0.0033(6) -0.0013(6) C12 0.0146(8) 0.0128(8) 0.0125(8) 0.0021(6) -0.0010(6) 0.0005(7) N11 0.0141(7) 0.0110(7) 0.0116(6) -0.0010(5) -0.0056(5) -0.0010(5) N9 0.0153(7) 0.0123(7) 0.0158(7) 0.0001(6) -0.0048(6) 0.0045(5) N8 0.0165(7) 0.0120(7) 0.0150(7) -0.0037(6) -0.0037(5) 0.0035(5) N14 0.0229(8) 0.0202(8) 0.0238(8) -0.0099(6) -0.0132(6) 0.0097(6) N13 0.0167(8) 0.0224(8) 0.0204(8) -0.0059(6) -0.0068(6) 0.0061(6) C3 0.0141(8) 0.0121(8) 0.0159(8) -0.0038(6) -0.0003(6) 0.0008(6) C5 0.0161(9) 0.0115(8) 0.0159(8) -0.0020(6) 0.0015(7) 0.0013(7) N4 0.0159(7) 0.0110(7) 0.0180(7) 0.0002(5) 0.0001(6) -0.0015(5) N1 0.0163(7) 0.0103(7) 0.0211(7) 0.0034(6) -0.0044(6) -0.0011(6) N2 0.0136(7) 0.0132(7) 0.0211(7) 0.0010(6) -0.0040(6) -0.0007(6) N6 0.0204(8) 0.0145(7) 0.0310(8) 0.0039(6) -0.0110(6) -0.0023(6) N7 0.0201(8) 0.0125(7) 0.0269(8) 0.0013(6) -0.0066(6) 0.0003(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 O1W H1W 0.7414 . ? O1W H2W 0.8159 . ? C10 N9 1.313(2) . ? C10 N14 1.339(2) . ? C10 N11 1.371(2) . ? C12 N8 1.315(2) . ? C12 N13 1.330(2) . ? C12 N11 1.348(2) . ? N11 H11A 0.7770 . ? N9 N8 1.3986(19) . ? N8 H8A 0.8036 . ? N14 H14A 0.8577 . ? N14 H14B 0.8320 . ? N13 H13A 0.8621 . ? N13 H13B 0.8192 . ? C3 N2 1.300(2) . ? C3 N7 1.356(2) . ? C3 N4 1.385(2) . ? C5 N6 1.320(2) . ? C5 N1 1.321(2) . ? C5 N4 1.350(2) . ? N4 H4A 0.8863 . ? N1 N2 1.3972(19) . ? N1 H1A 0.8021 . ? N6 H6A 0.8680 . ? N6 H6B 0.8352 . ? N7 H7B 0.8574 . ? N7 H7A 0.8476 . ? 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 H1W O1W H2W 99.6 . . ? N9 C10 N14 125.56(14) . . ? N9 C10 N11 111.25(14) . . ? N14 C10 N11 123.19(14) . . ? N8 C12 N13 127.58(15) . . ? N8 C12 N11 106.80(13) . . ? N13 C12 N11 125.58(15) . . ? C12 N11 C10 107.01(13) . . ? C12 N11 H11A 124.1 . . ? C10 N11 H11A 128.3 . . ? C10 N9 N8 103.54(13) . . ? C12 N8 N9 111.39(13) . . ? C12 N8 H8A 128.6 . . ? N9 N8 H8A 120.0 . . ? C10 N14 H14A 120.0 . . ? C10 N14 H14B 117.6 . . ? H14A N14 H14B 119.9 . . ? C12 N13 H13A 117.1 . . ? C12 N13 H13B 116.0 . . ? H13A N13 H13B 120.2 . . ? N2 C3 N7 126.06(15) . . ? N2 C3 N4 111.82(14) . . ? N7 C3 N4 122.02(15) . . ? N6 C5 N1 126.49(15) . . ? N6 C5 N4 126.81(15) . . ? N1 C5 N4 106.70(14) . . ? C5 N4 C3 106.31(13) . . ? C5 N4 H4A 126.6 . . ? C3 N4 H4A 125.3 . . ? C5 N1 N2 111.61(13) . . ? C5 N1 H1A 127.4 . . ? N2 N1 H1A 120.9 . . ? C3 N2 N1 103.55(13) . . ? C5 N6 H6A 123.2 . . ? C5 N6 H6B 117.0 . . ? H6A N6 H6B 118.8 . . ? C3 N7 H7B 110.4 . . ? C3 N7 H7A 116.6 . . ? H7B N7 H7A 116.6 . . ? _diffrn_measured_fraction_theta_max 0.987 _diffrn_reflns_theta_full 62.36 _diffrn_measured_fraction_theta_full 0.987 _refine_diff_density_max 0.233 _refine_diff_density_min -0.316 _refine_diff_density_rms 0.074 # Attachment '6003_web_deposit_cif_file_3_KarlaFejfarova_1309265877.dat_hclo4_precislovany.cif' data_dat_hclo4 _database_code_depnum_ccdc_archive 'CCDC 831899' #TrackingRef '6003_web_deposit_cif_file_3_KarlaFejfarova_1309265877.dat_hclo4_precislovany.cif' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety ? _chemical_formula_sum 'C4 H12 Cl2 N10 O8' _chemical_formula_weight 399.14 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' H H 0.0000 0.0000 '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' Cl Cl 0.3639 0.7018 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting ? _symmetry_space_group_name_H-M ? loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x, -y, -z' _cell_length_a 5.3075(2) _cell_length_b 7.5977(4) _cell_length_c 9.1610(5) _cell_angle_alpha 74.424(5) _cell_angle_beta 84.547(4) _cell_angle_gamma 83.648(4) _cell_volume 352.84(3) _cell_formula_units_Z 2 _cell_measurement_temperature 150(2) _cell_measurement_reflns_used ? _cell_measurement_theta_min ? _cell_measurement_theta_max ? _exptl_crystal_description ? _exptl_crystal_colour ? _exptl_crystal_size_max ? _exptl_crystal_size_mid ? _exptl_crystal_size_min ? _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 1.878 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 204 _exptl_absorpt_coefficient_mu 4.821 _exptl_absorpt_correction_type ? _exptl_absorpt_correction_T_min ? _exptl_absorpt_correction_T_max ? _exptl_absorpt_process_details ? _exptl_special_details ; ? ; _diffrn_ambient_temperature 150(2) _diffrn_radiation_wavelength 1.54178 _diffrn_radiation_type CuK\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 3565 _diffrn_reflns_av_R_equivalents 0.0186 _diffrn_reflns_av_sigmaI/netI 0.0124 _diffrn_reflns_limit_h_min -6 _diffrn_reflns_limit_h_max 6 _diffrn_reflns_limit_k_min -8 _diffrn_reflns_limit_k_max 8 _diffrn_reflns_limit_l_min -10 _diffrn_reflns_limit_l_max 10 _diffrn_reflns_theta_min 5.02 _diffrn_reflns_theta_max 62.32 _reflns_number_total 1098 _reflns_number_gt 1066 _reflns_threshold_expression >2sigma(I) _computing_data_collection ? _computing_cell_refinement ? _computing_data_reduction ? _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _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^)+(0.0415P)^2^+0.3835P] 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 mixed _refine_ls_extinction_method none _refine_ls_extinction_coef ? _refine_ls_number_reflns 1098 _refine_ls_number_parameters 133 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0284 _refine_ls_R_factor_gt 0.0278 _refine_ls_wR_factor_ref 0.0745 _refine_ls_wR_factor_gt 0.0741 _refine_ls_goodness_of_fit_ref 1.064 _refine_ls_restrained_S_all 1.064 _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 H4A H 0.050(5) 0.647(3) 0.705(3) 0.013(6) Uiso 1 1 d . . . H7A H -0.240(5) 0.805(4) 0.500(3) 0.018(7) Uiso 1 1 d . . . H7B H -0.399(5) 0.702(4) 0.456(3) 0.021(7) Uiso 1 1 d . . . H6B H 0.164(5) 0.241(4) 0.962(3) 0.016(7) Uiso 1 1 d . . . H1A H -0.198(5) 0.199(4) 0.811(3) 0.016(6) Uiso 1 1 d . . . H6A H 0.256(5) 0.413(4) 0.925(3) 0.026(7) Uiso 1 1 d . . . Cl1 Cl 0.37443(9) 0.86992(6) 0.80873(5) 0.01262(19) Uani 1 1 d . . . O2 O 0.2325(3) 0.8889(2) 0.67761(17) 0.0211(4) Uani 1 1 d . . . O1 O 0.4335(3) 0.67735(19) 0.87821(17) 0.0176(4) Uani 1 1 d . . . O3 O 0.2215(3) 0.9519(2) 0.91557(17) 0.0239(4) Uani 1 1 d . . . O4 O 0.6042(3) 0.9584(2) 0.76280(18) 0.0233(4) Uani 1 1 d . . . N4 N -0.0292(3) 0.5647(2) 0.70799(19) 0.0124(4) Uani 1 1 d . . . N1 N -0.1717(3) 0.3020(3) 0.77107(19) 0.0141(4) Uani 1 1 d . . . N2 N -0.3075(3) 0.4037(2) 0.64795(19) 0.0149(4) Uani 1 1 d . . . C5 C -0.0052(4) 0.3976(3) 0.8064(2) 0.0125(5) Uani 1 1 d . . . C3 C -0.2145(4) 0.5631(3) 0.6137(2) 0.0125(4) Uani 1 1 d . . . N7 N -0.2770(4) 0.7063(3) 0.4966(2) 0.0160(4) Uani 1 1 d . . . N6 N 0.1516(4) 0.3444(3) 0.9171(2) 0.0172(4) Uani 1 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 Cl1 0.0162(3) 0.0097(3) 0.0127(3) -0.00408(19) 0.00205(19) -0.00409(19) O2 0.0284(9) 0.0175(8) 0.0171(8) 0.0001(6) -0.0076(7) -0.0070(6) O1 0.0214(8) 0.0101(7) 0.0208(8) -0.0030(6) -0.0024(6) -0.0014(6) O3 0.0346(9) 0.0144(8) 0.0218(9) -0.0080(6) 0.0105(7) -0.0012(7) O4 0.0235(8) 0.0214(8) 0.0273(9) -0.0079(7) 0.0041(7) -0.0134(7) N4 0.0157(9) 0.0093(9) 0.0140(9) -0.0046(7) 0.0005(7) -0.0056(7) N1 0.0207(10) 0.0090(9) 0.0120(9) 0.0002(7) -0.0013(7) -0.0057(7) N2 0.0193(9) 0.0141(9) 0.0112(9) -0.0016(7) -0.0014(7) -0.0042(7) C5 0.0148(11) 0.0123(10) 0.0112(10) -0.0054(8) 0.0037(8) -0.0023(8) C3 0.0145(10) 0.0143(11) 0.0100(10) -0.0064(8) 0.0025(8) -0.0021(8) N7 0.0211(11) 0.0106(10) 0.0169(10) -0.0023(8) -0.0045(8) -0.0041(8) N6 0.0226(10) 0.0117(10) 0.0172(10) -0.0009(8) -0.0047(8) -0.0060(8) _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 Cl1 O4 1.4309(16) . ? Cl1 O3 1.4385(15) . ? Cl1 O1 1.4424(15) . ? Cl1 O2 1.4444(16) . ? N4 C5 1.346(3) . ? N4 C3 1.373(3) . ? N1 C5 1.317(3) . ? N1 N2 1.397(2) . ? N2 C3 1.307(3) . ? C5 N6 1.323(3) . ? C3 N7 1.344(3) . ? 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 O4 Cl1 O3 110.11(9) . . ? O4 Cl1 O1 109.87(9) . . ? O3 Cl1 O1 109.35(9) . . ? O4 Cl1 O2 109.65(9) . . ? O3 Cl1 O2 109.09(10) . . ? O1 Cl1 O2 108.75(9) . . ? C5 N4 C3 107.40(17) . . ? C5 N1 N2 112.11(17) . . ? C3 N2 N1 103.18(17) . . ? N1 C5 N6 127.91(19) . . ? N1 C5 N4 105.96(18) . . ? N6 C5 N4 126.12(19) . . ? N2 C3 N7 125.7(2) . . ? N2 C3 N4 111.35(18) . . ? N7 C3 N4 122.84(19) . . ? _diffrn_measured_fraction_theta_max 0.979 _diffrn_reflns_theta_full 62.32 _diffrn_measured_fraction_theta_full 0.979 _refine_diff_density_max 0.305 _refine_diff_density_min -0.380 _refine_diff_density_rms 0.055 # Attachment '6004_web_deposit_cif_file_4_KarlaFejfarova_1309265877.dat_hpo3_precislovany.cif' #============================================================================== data_dat_hpo3 _database_code_depnum_ccdc_archive 'CCDC 831900' #TrackingRef '6004_web_deposit_cif_file_4_KarlaFejfarova_1309265877.dat_hpo3_precislovany.cif' _cell_special_details ? #Added by publCIF _symmetry_space_group_name_hall '-P 2ybc' #Added by publCIF _audit_update_record ; 2010-04-26 # Formatted by publCIF ; _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'C2 H6 N5, H2 O3 P ' _chemical_formula_sum 'C2 H8 N5 O3 P' _chemical_formula_weight 181.10 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' H H 0.0000 0.0000 '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' P P 0.2955 0.4335 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting monoclinic _symmetry_space_group_name_H-M P2(1)/c loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x, y+1/2, -z+1/2' '-x, -y, -z' 'x, -y-1/2, z-1/2' _cell_length_a 8.16880(10) _cell_length_b 11.4624(2) _cell_length_c 7.74230(10) _cell_angle_alpha 90.00 _cell_angle_beta 96.1060(10) _cell_angle_gamma 90.00 _cell_volume 720.830(18) _cell_formula_units_Z 4 _cell_measurement_temperature 120(2) _cell_measurement_reflns_used 7111 _cell_measurement_theta_min 3.8532 _cell_measurement_theta_max 62.4539 _exptl_crystal_description plate _exptl_crystal_colour colourless _exptl_crystal_size_max 0.3956 _exptl_crystal_size_mid 0.2358 _exptl_crystal_size_min 0.1328 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 1.669 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 376 _exptl_absorpt_coefficient_mu 3.242 _exptl_absorpt_correction_T_min 0.08792 _exptl_absorpt_correction_T_max 1.00000 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_process_details ; CrysAlisPro, Oxford Diffraction Ltd., Version 1.171.33.55 ; _exptl_special_details ; ? ; _diffrn_ambient_temperature 120(2) _diffrn_radiation_wavelength 1.54184 _diffrn_radiation_type CuK\a _diffrn_radiation_source 'Enhance Ultra (Cu) X-ray Source' _diffrn_radiation_monochromator mirror _diffrn_measurement_device_type 'Xcalibur, Atlas, Gemini ultra' _diffrn_measurement_method 'Rotation method data acquisition using \w' _diffrn_detector_area_resol_mean 10.3784 _diffrn_standards_number ? _diffrn_standards_interval_count ? _diffrn_standards_interval_time ? _diffrn_standards_decay_% ? _diffrn_reflns_number 8465 _diffrn_reflns_av_R_equivalents 0.0339 _diffrn_reflns_av_sigmaI/netI 0.0145 _diffrn_reflns_limit_h_min -9 _diffrn_reflns_limit_h_max 9 _diffrn_reflns_limit_k_min -13 _diffrn_reflns_limit_k_max 13 _diffrn_reflns_limit_l_min -8 _diffrn_reflns_limit_l_max 8 _diffrn_reflns_theta_min 5.45 _diffrn_reflns_theta_max 62.55 _reflns_number_total 1137 _reflns_number_gt 1106 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'Crysalis CCD (Oxford Diffraction, 2007)' _computing_cell_refinement 'Crysalis RED (Oxford Diffraction, 2007)' _computing_data_reduction 'Crysalis RED (Oxford Diffraction, 2007)' _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics ? _computing_publication_material 'publCIF (MacMahon, 2008)' _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. The hydrogen atoms could be localized from the difference Fourier map. Despite of that, all hydrogen atoms, except H1A, H1 and H2, were constrained to ideal positions. The N---H distances were not restrained. ; _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^)+(0.0423P)^2^+1.0464P] 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 SHELXL _refine_ls_extinction_coef 0.0078(6) _refine_ls_extinction_expression Fc^*^=kFc[1+0.001xFc^2^\l^3^/sin(2\q)]^-1/4^ _refine_ls_number_reflns 1137 _refine_ls_number_parameters 101 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0286 _refine_ls_R_factor_gt 0.0281 _refine_ls_wR_factor_ref 0.0718 _refine_ls_wR_factor_gt 0.0714 _refine_ls_goodness_of_fit_ref 0.883 _refine_ls_restrained_S_all 0.883 _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 H1A H 0.6143 0.4398 0.8607 0.050 Uiso 1 1 d . . . H2 H 1.0267 0.3442 0.8127 0.050 Uiso 1 1 d . . . H1 H 0.9447 0.3855 1.1682 0.050 Uiso 1 1 d . . . H7A H 0.1509 0.5573 0.4657 0.050 Uiso 1 1 d . . . H7B H 0.1569 0.4295 0.5061 0.050 Uiso 1 1 d . . . C3 C 0.3370(2) 0.50518(15) 0.6202(2) 0.0142(4) Uani 1 1 d . . . C5 C 0.5332(2) 0.59276(15) 0.7862(2) 0.0148(4) Uani 1 1 d . . . N7 N 0.20705(19) 0.49184(13) 0.4983(2) 0.0194(4) Uani 1 1 d . . . N4 N 0.40276(18) 0.61269(13) 0.66740(19) 0.0141(3) Uani 1 1 d . . . H4A H 0.3676 0.6795 0.6288 0.022 Uiso 1 1 calc . . . N6 N 0.6302(2) 0.67309(14) 0.8648(2) 0.0225(4) Uani 1 1 d . . . H6B H 0.7101 0.6529 0.9403 0.033 Uiso 1 1 calc . . . H6A H 0.6136 0.7456 0.8406 0.030 Uiso 1 1 calc . . . N1 N 0.54253(18) 0.47840(13) 0.8089(2) 0.0162(3) Uani 1 1 d . . . N2 N 0.41924(18) 0.42067(13) 0.70266(19) 0.0159(4) Uani 1 1 d . . . O1 O 0.75288(15) 0.31457(10) 0.95478(17) 0.0185(3) Uani 1 1 d . . . O2 O 1.04899(15) 0.37061(11) 0.91808(16) 0.0184(3) Uani 1 1 d . . . O3 O 0.99092(15) 0.19540(11) 1.09951(16) 0.0174(3) Uani 1 1 d . . . P1 P 0.92732(5) 0.31383(4) 1.03886(6) 0.01345(19) Uani 1 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 C3 0.0135(9) 0.0127(9) 0.0166(9) -0.0006(7) 0.0033(7) -0.0011(7) C5 0.0130(9) 0.0124(9) 0.0191(9) 0.0008(7) 0.0019(7) 0.0009(7) N7 0.0182(8) 0.0138(8) 0.0246(8) 0.0012(6) -0.0053(6) -0.0025(6) N4 0.0134(7) 0.0089(7) 0.0196(8) 0.0019(6) -0.0004(6) 0.0010(6) N6 0.0192(8) 0.0129(8) 0.0323(10) 0.0023(7) -0.0110(7) -0.0002(6) N1 0.0134(8) 0.0120(8) 0.0219(8) 0.0012(6) -0.0038(6) 0.0011(6) N2 0.0142(8) 0.0128(8) 0.0201(8) -0.0001(6) -0.0017(6) -0.0009(6) O1 0.0151(7) 0.0120(6) 0.0269(7) 0.0002(5) -0.0042(5) 0.0007(5) O2 0.0185(7) 0.0197(7) 0.0160(6) -0.0005(5) -0.0029(5) -0.0046(5) O3 0.0186(7) 0.0147(7) 0.0180(7) 0.0003(5) -0.0023(5) 0.0030(5) P1 0.0129(3) 0.0115(3) 0.0151(3) -0.00099(16) -0.00243(18) 0.00075(16) _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 C3 N2 1.306(2) . ? C3 N7 1.352(2) . ? C3 N4 1.378(2) . ? C5 N6 1.321(2) . ? C5 N1 1.324(2) . ? C5 N4 1.351(2) . ? N7 H7A 0.9011 . ? N7 H7B 0.8296 . ? N4 H4A 0.8600 . ? N6 H6B 0.8600 . ? N6 H6A 0.8600 . ? N1 N2 1.397(2) . ? N1 H1A 0.8069 . ? O1 P1 1.5023(13) . ? O2 P1 1.5759(13) . ? O2 H2 0.8714 . ? O3 P1 1.5104(13) . ? P1 H1 1.2918 . ? 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 N2 C3 N7 125.61(16) . . ? N2 C3 N4 111.58(15) . . ? N7 C3 N4 122.76(16) . . ? N6 C5 N1 127.28(17) . . ? N6 C5 N4 125.97(16) . . ? N1 C5 N4 106.75(15) . . ? C3 N7 H7A 116.1 . . ? C3 N7 H7B 113.8 . . ? H7A N7 H7B 119.8 . . ? C5 N4 C3 106.63(14) . . ? C5 N4 H4A 126.7 . . ? C3 N4 H4A 126.7 . . ? C5 N6 H6B 120.0 . . ? C5 N6 H6A 120.0 . . ? H6B N6 H6A 120.0 . . ? C5 N1 N2 111.28(15) . . ? C5 N1 H1A 129.7 . . ? N2 N1 H1A 118.2 . . ? C3 N2 N1 103.75(14) . . ? P1 O2 H2 109.3 . . ? O1 P1 O3 114.76(7) . . ? O1 P1 O2 111.69(7) . . ? O3 P1 O2 109.75(7) . . ? O1 P1 H1 110.7 . . ? O3 P1 H1 109.0 . . ? O2 P1 H1 100.0 . . ? _diffrn_measured_fraction_theta_max 0.994 _diffrn_reflns_theta_full 62.55 _diffrn_measured_fraction_theta_full 0.994 _refine_diff_density_max 0.358 _refine_diff_density_min -0.352 _refine_diff_density_rms 0.066 # Attachment '6005_web_deposit_cif_file_5_KarlaFejfarova_1309265877.dat_no3_1_precislovany.cif' data_dat_no3_1 _database_code_depnum_ccdc_archive 'CCDC 831901' #TrackingRef '6005_web_deposit_cif_file_5_KarlaFejfarova_1309265877.dat_no3_1_precislovany.cif' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety ? _chemical_formula_sum 'C8 H24 N44 O12' _chemical_formula_weight 648.51 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' H H 0.0000 0.0000 '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' _symmetry_cell_setting monoclinic _symmetry_space_group_name_H-M P21/c loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x, y+1/2, -z+1/2' '-x, -y, -z' 'x, -y-1/2, z-1/2' _cell_length_a 9.51950(10) _cell_length_b 9.10000(10) _cell_length_c 7.41270(10) _cell_angle_alpha 90.00 _cell_angle_beta 95.9880(10) _cell_angle_gamma 90.00 _cell_volume 638.640(13) _cell_formula_units_Z 4 _cell_measurement_temperature 120(2) _cell_measurement_reflns_used 4542 _cell_measurement_theta_min 4.6668 _cell_measurement_theta_max 62.3029 _exptl_crystal_description yellowish _exptl_crystal_colour plate _exptl_crystal_size_max 0.4260 _exptl_crystal_size_mid 0.2800 _exptl_crystal_size_min 0.1837 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 1.686 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 336 _exptl_absorpt_coefficient_mu 1.336 _exptl_absorpt_correction_type multiscan _exptl_absorpt_correction_T_min 0.18263 _exptl_absorpt_correction_T_max 1.0000 _exptl_absorpt_process_details ? _exptl_special_details ; CrysAlisPro, Oxford Diffraction Ltd., Version 1.171.33.55 (release 05-01-2010 CrysAlis171 .NET) (compiled Jan 5 2010,16:28:46) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm. ; _diffrn_ambient_temperature 150(2) _diffrn_radiation_wavelength 1.54178 _diffrn_radiation_type CuK\a _diffrn_radiation_source 'Enhance Ultra (Cu) X-ray Source' _diffrn_radiation_monochromator minor _diffrn_measurement_device_type 'Xcalibur, Atlas, Gemini ultra' _diffrn_measurement_method ? _diffrn_detector_area_resol_mean 10.3784 _diffrn_standards_number ? _diffrn_standards_interval_count ? _diffrn_standards_interval_time ? _diffrn_standards_decay_% ? _diffrn_reflns_number 4685 _diffrn_reflns_av_R_equivalents 0.0293 _diffrn_reflns_av_sigmaI/netI 0.0156 _diffrn_reflns_limit_h_min -10 _diffrn_reflns_limit_h_max 10 _diffrn_reflns_limit_k_min -10 _diffrn_reflns_limit_k_max 10 _diffrn_reflns_limit_l_min -8 _diffrn_reflns_limit_l_max 8 _diffrn_reflns_theta_min 4.67 _diffrn_reflns_theta_max 62.39 _reflns_number_total 1011 _reflns_number_gt 969 _reflns_threshold_expression >2sigma(I) _computing_data_collection ; CrysAlisPro, Oxford Diffraction Ltd., Version 1.171.33.55 (release 05-01-2010 CrysAlis171 .NET) (compiled Jan 5 2010,16:28:46) ; _computing_cell_refinement ; CrysAlisPro, Oxford Diffraction Ltd., Version 1.171.33.55 (release 05-01-2010 CrysAlis171 .NET) (compiled Jan 5 2010,16:28:46) ; _computing_data_reduction ; CrysAlisPro, Oxford Diffraction Ltd., Version 1.171.33.55 (release 05-01-2010 CrysAlis171 .NET) (compiled Jan 5 2010,16:28:46) ; _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _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^)+(0.0457P)^2^+0.2247P] 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 mixed _refine_ls_extinction_method none _refine_ls_extinction_coef ? _refine_ls_number_reflns 1011 _refine_ls_number_parameters 124 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0293 _refine_ls_R_factor_gt 0.0281 _refine_ls_wR_factor_ref 0.0781 _refine_ls_wR_factor_gt 0.0769 _refine_ls_goodness_of_fit_ref 1.117 _refine_ls_restrained_S_all 1.117 _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 H6B H -0.4594(19) 0.567(2) -0.674(3) 0.027(4) Uiso 1 1 d . . . H7A H 0.0158(19) 0.779(2) -0.219(2) 0.030(5) Uiso 1 1 d . . . H4A H -0.2238(19) 0.797(2) -0.419(2) 0.032(5) Uiso 1 1 d . . . H6A H -0.4357(19) 0.726(2) -0.619(2) 0.034(5) Uiso 1 1 d . . . H7B H 0.072(2) 0.630(2) -0.166(3) 0.034(5) Uiso 1 1 d . . . H1A H -0.2756(18) 0.381(2) -0.501(2) 0.024(4) Uiso 1 1 d . . . O3 O 0.40473(10) 0.45275(10) 0.14206(12) 0.0173(3) Uani 1 1 d . . . O1 O 0.34633(10) 0.67973(10) 0.08810(13) 0.0222(3) Uani 1 1 d . . . O2 O 0.24683(10) 0.50557(10) -0.08069(13) 0.0215(3) Uani 1 1 d . . . N3 N 0.33251(11) 0.54713(12) 0.05009(15) 0.0148(3) Uani 1 1 d . . . N7 N -0.00002(13) 0.68362(15) -0.20986(18) 0.0248(3) Uani 1 1 d . . . N6 N -0.41749(12) 0.63063(15) -0.60247(17) 0.0195(3) Uani 1 1 d . . . N4 N -0.21116(12) 0.69707(13) -0.41309(14) 0.0155(3) Uani 1 1 d . . . N2 N -0.11677(12) 0.47805(13) -0.34852(15) 0.0177(3) Uani 1 1 d . . . C3 C -0.10232(13) 0.61917(15) -0.32006(18) 0.0156(3) Uani 1 1 d . . . N1 N -0.24065(12) 0.46764(13) -0.46782(15) 0.0162(3) Uani 1 1 d . . . C5 C -0.29748(13) 0.59812(14) -0.50344(17) 0.0143(3) Uani 1 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 O3 0.0179(5) 0.0123(5) 0.0207(5) 0.0027(4) -0.0024(4) 0.0032(4) O1 0.0257(6) 0.0103(5) 0.0294(5) -0.0003(4) -0.0035(4) 0.0001(4) O2 0.0204(5) 0.0179(5) 0.0241(6) -0.0019(4) -0.0082(4) 0.0003(4) N3 0.0135(6) 0.0121(6) 0.0186(6) 0.0011(4) 0.0013(5) -0.0003(4) N7 0.0198(7) 0.0126(7) 0.0391(8) -0.0005(6) -0.0106(6) 0.0008(5) N6 0.0200(7) 0.0124(7) 0.0246(7) -0.0008(5) -0.0049(5) -0.0002(5) N4 0.0147(6) 0.0102(6) 0.0211(6) -0.0001(5) 0.0001(5) -0.0006(4) N2 0.0140(6) 0.0149(7) 0.0233(6) -0.0015(5) -0.0024(5) -0.0001(4) C3 0.0139(7) 0.0123(7) 0.0207(7) 0.0003(5) 0.0018(5) 0.0000(5) N1 0.0154(6) 0.0116(6) 0.0211(6) -0.0017(5) -0.0016(5) -0.0006(5) C5 0.0148(7) 0.0124(7) 0.0158(6) 0.0000(5) 0.0025(5) -0.0012(5) _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 O3 N3 1.2559(14) . ? O1 N3 1.2430(15) . ? O2 N3 1.2583(14) . ? N7 C3 1.3392(18) . ? N6 C5 1.3254(18) . ? N4 C5 1.3489(17) . ? N4 C3 1.3793(17) . ? N2 C3 1.3064(19) . ? N2 N1 1.4015(16) . ? N1 C5 1.3200(18) . ? 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 N3 O3 120.12(11) . . ? O1 N3 O2 120.75(11) . . ? O3 N3 O2 119.13(11) . . ? C5 N4 C3 106.98(12) . . ? C3 N2 N1 103.64(11) . . ? N2 C3 N7 125.92(13) . . ? N2 C3 N4 111.32(12) . . ? N7 C3 N4 122.71(13) . . ? C5 N1 N2 111.45(11) . . ? N1 C5 N6 128.54(13) . . ? N1 C5 N4 106.58(12) . . ? N6 C5 N4 124.84(13) . . ? _diffrn_measured_fraction_theta_max 0.992 _diffrn_reflns_theta_full 62.39 _diffrn_measured_fraction_theta_full 0.992 _refine_diff_density_max 0.177 _refine_diff_density_min -0.219 _refine_diff_density_rms 0.046 # Attachment '6006_web_deposit_cif_file_6_KarlaFejfarova_1309265877.dat-h3po4_1_precislovany.cif' #======================================================================= data_III _database_code_depnum_ccdc_archive 'CCDC 831902' #TrackingRef '6006_web_deposit_cif_file_6_KarlaFejfarova_1309265877.dat-h3po4_1_precislovany.cif' #======================================================================= # 5. CHEMICAL DATA _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_formula_moiety 'C2 H6 N5, H2 O4 P ' _chemical_formula_structural ? _chemical_formula_analytical ? _chemical_formula_iupac ? _chemical_formula_sum 'C2 H8 N5 O4 P1' _chemical_formula_weight 197.1 _chemical_melting_point ? _chemical_compound_source ? _chemical_absolute_configuration ad #======================================================================= # 6. CRYSTAL DATA _symmetry_cell_setting orthorhombic _symmetry_space_group_name_H-M 'F d d 2' _symmetry_space_group_name_Hall 'F 2 -2d' loop_ _symmetry_equiv_pos_site_id _symmetry_equiv_pos_as_xyz 1 x,y,z 2 -x,-y,z 3 x+1/4,-y+1/4,z+1/4 4 -x+1/4,y+1/4,z+1/4 5 x,y+1/2,z+1/2 6 -x,-y+1/2,z+1/2 7 x+1/4,-y+3/4,z+3/4 8 -x+1/4,y+3/4,z+3/4 9 x+1/2,y,z+1/2 10 -x+1/2,-y,z+1/2 11 x+3/4,-y+1/4,z+3/4 12 -x+3/4,y+1/4,z+3/4 13 x+1/2,y+1/2,z 14 -x+1/2,-y+1/2,z 15 x+3/4,-y+3/4,z+1/4 16 -x+3/4,y+3/4,z+1/4 _cell_length_a 13.3492(4) _cell_length_b 37.1096(12) _cell_length_c 6.0702(2) _cell_angle_alpha 90 _cell_angle_beta 90 _cell_angle_gamma 90 _cell_volume 3007.08(17) _cell_formula_units_Z 16 _cell_measurement_reflns_used 7644 _cell_measurement_theta_min 4.7671 _cell_measurement_theta_max 66.6468 _cell_measurement_temperature 120 _cell_special_details ; ? ; _exptl_crystal_density_diffrn 1.7408 _exptl_crystal_density_meas ? _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 1632 _exptl_absorpt_coefficient_mu 3.270 _exptl_crystal_description 'irregular shape' _exptl_crystal_size_max 0.3851 _exptl_crystal_size_mid 0.2734 _exptl_crystal_size_min 0.1800 _exptl_crystal_colour colorless _exptl_absorpt_correction_T_min 0.485 _exptl_absorpt_correction_T_max 0.686 _exptl_absorpt_correction_type analytical _exptl_absorpt_process_details ; CrysAlisPro, Oxford Diffraction Ltd., Version 1.171.33.51 (release 27-10-2009 CrysAlis171 .NET) Analytical numeric absorption correction using a multifaceted crystal model based on expressions derived by R.C. Clark & J.S. Reid. ; #======================================================================= # 7. EXPERIMENTAL DATA _exptl_special_details ? _diffrn_ambient_temperature 120 _diffrn_radiation_type 'Cu K\a' _diffrn_radiation_source 'X-ray tube' _diffrn_radiation_wavelength 1.54184 _diffrn_radiation_monochromator mirror _diffrn_measurement_device 'four-cycle diffractometer' _diffrn_measurement_device_type 'Goniometer Xcalibur, detector: Atlas (Gemini ultra Cu)' _diffrn_detector_area_resol_mean 10.3784 _diffrn_measurement_method 'Rotation method data acquisition using \w scans' _diffrn_reflns_number 8122 _diffrn_reflns_theta_min 7.05 _diffrn_reflns_theta_max 66.79 _diffrn_reflns_theta_full 66.79 _diffrn_measured_fraction_theta_max 0.99 _diffrn_measured_fraction_theta_full 0.99 _diffrn_reflns_av_R_equivalents 0.0247 _diffrn_reflns_av_sigmaI/netI 0.0055 _diffrn_reflns_limit_h_min -15 _diffrn_reflns_limit_h_max 15 _diffrn_reflns_limit_k_min -42 _diffrn_reflns_limit_k_max 44 _diffrn_reflns_limit_l_min -7 _diffrn_reflns_limit_l_max 6 _diffrn_reflns_reduction_process ; Integration of the CCD images was done by program Crysalis RED (Oxford diffraction, 2008). The same program was used for indexing of the crystal shape and absorption correction. ; #======================================================================= # 8. REFINEMENT DATA _refine_special_details ; The refinement was carried out against all reflections. The conventional R-factor is always based on F. The goodness of fit as well as the weighted R-factor are based on F and F^2^ for refinement carried out on F and F^2^, respectively. The threshold expression is used only for calculating R-factors etc. and it is not relevant to the choice of reflections for refinement. The program used for refinement, Jana2006, uses the weighting scheme based on the experimental expectations, see _refine_ls_weighting_details, that does not force S to be one. Therefore the values of S are usually larger than the ones from the SHELX program. ; _reflns_number_total 1295 _reflns_number_gt 1290 _reflns_threshold_expression I>3\s(I) _refine_ls_structure_factor_coef Fsqd _refine_ls_R_factor_gt 0.0189 _refine_ls_wR_factor_gt 0.0615 _refine_ls_R_factor_all 0.0190 _refine_ls_wR_factor_ref 0.0617 _refine_ls_goodness_of_fit_ref 1.52 _refine_ls_goodness_of_fit_gt 1.52 _refine_ls_restrained_S_gt ? _refine_ls_restrained_S_all ? _refine_ls_number_reflns 1295 _refine_ls_number_parameters 133 _refine_ls_number_restraints 8 _refine_ls_number_constraints 9 _refine_ls_weighting_scheme sigma _refine_ls_weighting_details w=1/(\s^2^(I)+0.0016I^2^) _refine_ls_hydrogen_treatment refxyz _refine_ls_shift/su_max 0.0100 _refine_ls_shift/su_mean 0.0013 _refine_diff_density_max 0.09 _refine_diff_density_min -0.11 _refine_ls_extinction_method 'B-C type 1 Lorentzian isotropic (Becker & Coppens, 1974)' _refine_ls_extinction_coef 1900(200) _refine_ls_abs_structure_details 'Flack (1983)' _refine_ls_abs_structure_Flack 0.034(16) _refine_ls_abs_structure_Rogers ? loop_ _atom_type_symbol _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source C 0.018 0.009 'International Tables Vol C tables 4.2.6.8 and 6.1.1.1' H 0.000 0.000 'International Tables Vol C tables 4.2.6.8 and 6.1.1.1' N 0.031 0.018 'International Tables Vol C tables 4.2.6.8 and 6.1.1.1' O 0.049 0.032 'International Tables Vol C tables 4.2.6.8 and 6.1.1.1' P 0.296 0.433 'International Tables Vol C tables 4.2.6.8 and 6.1.1.1' _computing_data_collection 'Crysalis CCD (Oxford diffraction, 2009)' _computing_cell_refinement 'Crysalis RED (Oxford diffraction, 2009)' _computing_data_reduction 'Crysalis RED' _computing_structure_solution 'SIR2002 (Burla et al., 2003)' _computing_structure_refinement "Jana2006 (Pet\