# Supplementary Material (ESI) for Chemical Communications # This journal is © The Royal Society of Chemistry 2004 data_global _journal_name_full Chem.Commun. _journal_coden_Cambridge 0182 _publ_contact_author_name 'Prof Jing-Tai Zhao' _publ_contact_author_address ; State Key Laboratory of High Performance and Superfine Microstructure Shanghai Institute of Ceramics Chinese Academy of Scienc Shanghai CHINA ; _publ_contact_author_email JTZHAO@MAIL.SIC.AC.CN _publ_section_title ; NH4[BPO4F]: A Novel Open-Framework Ammonium Fluorinated Borophosphate With a Zeolite-Like Structure Related to Gismondine Topology ; loop_ _publ_author_name 'Jingtai Zhao' 'Chen Hao-Hong' 'Ge Ming-Hui' 'Li Man-Rong' 'Liu Wei' ; Yang Xin-Xin ; data_nd _database_code_depnum_ccdc_archive 'CCDC 232990' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'B2 F2 O8 P2,2(H4 N)' _chemical_formula_sum 'H8 B2 F2 N2 O8 P2' _chemical_formula_weight 285.64 loop_ _atom_type_symbol _atom_type_description _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source B B 0.0013 0.0007 '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' O O 0.0106 0.0060 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' P P 0.1023 0.0942 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' F F 0.0171 0.0103 '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' _symmetry_cell_setting cubic _symmetry_space_group_name_H-M P213 loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x+1/2, -y, z+1/2' '-x, y+1/2, -z+1/2' 'x+1/2, -y+1/2, -z' 'z, x, y' 'z+1/2, -x+1/2, -y' '-z+1/2, -x, y+1/2' '-z, x+1/2, -y+1/2' 'y, z, x' '-y, z+1/2, -x+1/2' 'y+1/2, -z+1/2, -x' '-y+1/2, -z, x+1/2' _cell_length_a 7.5913(9) _cell_length_b 7.5913(9) _cell_length_c 7.5913(9) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 437.47(9) _cell_formula_units_Z 2 _cell_measurement_temperature 293(2) _cell_measurement_reflns_used 244 _cell_measurement_theta_min 3.80 _cell_measurement_theta_max 26.99 _exptl_crystal_description 'truncated cube' _exptl_crystal_colour colorless _exptl_crystal_size_max 0.02 _exptl_crystal_size_mid 0.02 _exptl_crystal_size_min 0.02 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 2.168 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 288 _exptl_absorpt_coefficient_mu 0.567 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_correction_T_min 0.9794 _exptl_absorpt_correction_T_max 0.9794 _exptl_absorpt_process_details sadabs _exptl_special_details ; ? ; _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 2207 _diffrn_reflns_av_R_equivalents 0.0598 _diffrn_reflns_av_sigmaI/netI 0.0922 _diffrn_reflns_limit_h_min -9 _diffrn_reflns_limit_h_max 8 _diffrn_reflns_limit_k_min -9 _diffrn_reflns_limit_k_max 9 _diffrn_reflns_limit_l_min -9 _diffrn_reflns_limit_l_max 5 _diffrn_reflns_theta_min 3.80 _diffrn_reflns_theta_max 26.99 _reflns_number_total 330 _reflns_number_gt 224 _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^)+(0.0251P)^2^+0.0000P] 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_abs_structure_details 'Flack H D (1983), Acta Cryst. A39, 876-881' _refine_ls_abs_structure_Flack 1.0(3) _refine_ls_number_reflns 330 _refine_ls_number_parameters 25 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0539 _refine_ls_R_factor_gt 0.0343 _refine_ls_wR_factor_ref 0.0656 _refine_ls_wR_factor_gt 0.0644 _refine_ls_goodness_of_fit_ref 0.854 _refine_ls_restrained_S_all 0.854 _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 P1 P 0.10009(11) 0.39991(11) 0.60009(11) 0.0284(4) Uani 1 3 d S . . F1 F 0.2610(3) 0.2610(3) 0.2610(3) 0.0494(10) Uani 1 3 d S . . O1 O 0.2948(3) 0.3905(3) 0.5433(2) 0.0326(6) Uani 1 1 d . . . O2 O -0.0126(3) 0.5126(3) 0.4874(3) 0.0406(11) Uani 1 3 d S . . B1 B 0.3665(5) 0.3665(5) 0.3665(5) 0.0348(19) Uani 1 3 d S . . N1 N 0.1300(3) 0.8700(3) 0.3700(3) 0.0419(13) Uani 1 3 d S . . H1 H 0.2476 0.8959 0.4211 0.050 Uiso 1 1 d . . . H2 H 0.0422 0.9578 0.4578 0.050 Uiso 1 3 d S . . 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 P1 0.0284(4) 0.0284(4) 0.0284(4) 0.0006(5) -0.0006(5) 0.0006(5) F1 0.0494(10) 0.0494(10) 0.0494(10) -0.0094(12) -0.0094(12) -0.0094(12) O1 0.0271(12) 0.0427(13) 0.0280(13) -0.0010(14) 0.0013(10) -0.0015(14) O2 0.0406(11) 0.0406(11) 0.0406(11) 0.0065(12) -0.0065(12) 0.0065(12) B1 0.0348(19) 0.0348(19) 0.0348(19) -0.004(2) -0.004(2) -0.004(2) N1 0.0419(13) 0.0419(13) 0.0419(13) -0.0018(15) 0.0018(15) 0.0018(15) _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 P1 O2 1.482(3) . ? P1 O1 1.541(2) 12_565 ? P1 O1 1.541(2) 6_456 ? P1 O1 1.541(2) . ? F1 B1 1.387(7) . ? O1 B1 1.460(3) . ? B1 O1 1.460(3) 5 ? B1 O1 1.460(3) 9 ? 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 O2 P1 O1 114.78(9) . 12_565 ? O2 P1 O1 114.78(9) . 6_456 ? O1 P1 O1 103.69(10) 12_565 6_456 ? O2 P1 O1 114.78(9) . . ? O1 P1 O1 103.69(10) 12_565 . ? O1 P1 O1 103.69(10) 6_456 . ? B1 O1 P1 128.3(3) . . ? F1 B1 O1 112.8(3) . . ? F1 B1 O1 112.8(3) . 5 ? O1 B1 O1 105.9(3) . 5 ? F1 B1 O1 112.8(3) . 9 ? O1 B1 O1 105.9(3) . 9 ? O1 B1 O1 105.9(3) 5 9 ? _diffrn_measured_fraction_theta_max 1.000 _diffrn_reflns_theta_full 26.99 _diffrn_measured_fraction_theta_full 1.000 _refine_diff_density_max 0.169 _refine_diff_density_min -0.184 _refine_diff_density_rms 0.051