# Electronic Supplementary Material (ESI) for Dalton Transactions # This journal is © The Royal Society of Chemistry 2012 #Added by publCIF data_New_Global_Publ_Block _journal_name_full 'Dalton Trans.' _journal_coden_cambridge 0222 #TrackingRef '- GePO-1 (CSD-424507)-revised.cif' _publ_section_related_literature ? # Added by publCIF - use a unique identifier for each data block #============================================================================== # SUBMISSION DETAILS _publ_contact_author_name 'Lei Liu' # Name of author for correspondence _publ_contact_author_address # Address of author for correspondence ; Research Institute of Special Chemicals, Taiyuan University of Technology, Taiyuan030024,China. ; _publ_contact_author_email liulei@tyut.edu.cn _publ_contact_author_fax 86-351-6111178 _publ_contact_author_phone 86-3516010550-5 _publ_contact_letter ; Please consider this CIF for publication. I certify that this contibution is the original work of those listed as authors; that it has not been published before (in any language or medium) and is not being considered for publication elsewhere; that all authors concur with and are aware of the submission; that all workers involved in the study are listed as authors or given proper credit in the acknowledgements; that I have obtained permission for and acknowledged the source of any excerpts from other copyright works; and that to the best of my knowledge the paper contains no statements which are libellous, unlawful or in any way actionable. All coauthors have made significant scientific contributions to the work reported, including the ideas and their execution, and share responsibility and accountability for the results. ; _publ_requested_category ? #============================================================================== # TITLE AND AUTHOR LIST _publ_section_title ; The first ionothermal synthesis of a germanium phosphate with one-dimensional chain structure ; _publ_section_title_footnote # remove if not required . # The loop structure below should contain the names and addresses of all # authors, in the required order of publication. Repeat as necessary. # NB if using publCIF, the Author database tool might prove useful # (see the Tools menu in publCIF) loop_ _publ_author_name _publ_author_address _publ_author_footnote 'Wei Wang' ; Research Institute of Special Chemicals, Taiyuan University of Technology, Taiyuan030024,China. ; . 'Yang Li' ; University of St Andrews,Purdie Building,St Andrews KY16 9ST, UK ; . 'Lei Liu' ; Research Institute of Special Chemicals, Taiyuan University of Technology, Taiyuan030024,China. ; . 'Jinxiang Dong' ; Research Institute of Special Chemicals, Taiyuan University of Technology, Taiyuan030024,China. ; . #============================================================================== # TEXT _publ_section_synopsis . _publ_section_abstract ; (type here to add abstract) ; _publ_section_comment ; The stucture of the title compound, (I), is shown below. Dimensions are available in the archived CIF. For related literature, see [type here to add references to related literature]. ; _publ_section_acknowledgements # remove if not required ; (type here to add acknowledgements) ; _publ_section_references ; ? ; _publ_section_figure_captions ; ; _publ_section_exptl_prep ; (type here to add preparation details) ; _publ_section_exptl_refinement ; (type here to add refinement details) ; #============================================================================== _publ_manuscript_text # Used for convenience to store draft or replaced versions # of the abstract, comment etc. # Its contents will not be output ; ? ; #============================================================================== # Formatted by publCIF data_GePO-1 _database_code_depnum_ccdc_archive 'CCDC 877718' #TrackingRef '- GePO-1 (CSD-424507)-revised.cif' _audit_update_record ; 2012-04-06 # Formatted by publCIF ; _audit_creation_method SHELXL-97 _chemical_name_systematic ; ; _chemical_name_common TG27 _chemical_melting_point ? _chemical_formula_moiety 'Ge H6 N2 O8 P2, 2(H4 N), 0.38(H2 O)' _chemical_formula_sum 'Ge H14.77 N4 O8.38 P2' _chemical_formula_weight 340.8839 loop_ _atom_type_symbol _atom_type_description _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source Ge Ge 0.1547 1.8001 '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' P P 0.1023 0.0942 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting Monoclinic _symmetry_space_group_name_H-M C2/m loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x, y, -z' 'x+1/2, y+1/2, z' '-x+1/2, y+1/2, -z' '-x, -y, -z' 'x, -y, z' '-x+1/2, -y+1/2, -z' 'x+1/2, -y+1/2, z' _cell_length_a 10.644(4) _cell_length_b 5.1233(19) _cell_length_c 10.309(3) _cell_angle_alpha 90.00 _cell_angle_beta 106.622(10) _cell_angle_gamma 90.00 _cell_volume 538.7(3) _cell_formula_units_Z 2 _cell_measurement_temperature 93(2) _cell_measurement_reflns_used 1135 _cell_measurement_theta_min 3.9957 _cell_measurement_theta_max 28.1382 _exptl_crystal_description Prism _exptl_crystal_colour Colorless _exptl_crystal_size_max 0.10 _exptl_crystal_size_mid 0.04 _exptl_crystal_size_min 0.02 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 2.100 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 344 _exptl_absorpt_coefficient_mu 3.179 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_correction_T_min 0.7416 _exptl_absorpt_correction_T_max 0.9391 _exptl_absorpt_process_details '(CrystalClear; Rigaku,2004)' _exptl_special_details ; ? ; _diffrn_ambient_temperature 93(2) _diffrn_radiation_wavelength 0.71073 _diffrn_radiation_type MoK\a _diffrn_radiation_source 'rotating anode' _diffrn_radiation_monochromator confocal _diffrn_measurement_device_type CCD _diffrn_measurement_method dtprofit.ref _diffrn_detector_area_resol_mean 0.83 _diffrn_standards_number ? _diffrn_standards_interval_count ? _diffrn_standards_interval_time ? _diffrn_standards_decay_% ? _diffrn_reflns_number 1869 _diffrn_reflns_av_R_equivalents 0.0123 _diffrn_reflns_av_sigmaI/netI 0.0132 _diffrn_reflns_limit_h_min -11 _diffrn_reflns_limit_h_max 12 _diffrn_reflns_limit_k_min -3 _diffrn_reflns_limit_k_max 6 _diffrn_reflns_limit_l_min -10 _diffrn_reflns_limit_l_max 12 _diffrn_reflns_theta_min 4.00 _diffrn_reflns_theta_max 28.46 _reflns_number_total 627 _reflns_number_gt 615 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'CrystalClear (Rigaku Corp., 2004)' _computing_cell_refinement 'CrystalClear (Rigaku Corp., 2004)' _computing_data_reduction 'CrystalClear (Rigaku Corp., 2004)' _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics PLATON(Spek,2003) _computing_publication_material 'Bruker SHELXTL' _refine_special_details ; All the N-H bond distances were restrained to a 0.98\%A with a default standard deviation 0.03\%A in the refinement. The hydrogen atom of solvent water molecule was not found on the solvent water molecule, and therefore, is not included in the final structure. The isolated water molecule is strongly disordered and partially occupied, and therefore, the O atom was refined anisotropically and the occupancy of O atom was refined using a free variable. The refinement was not able to determine definitely the isolated solvent molecule was water rather than NH3 because the different assignments(O or N a tom) of isolated molecule result in nearly the same R factor and the same size of the ADP. However,the element analysis and the chemical possibility suggested the isolated molecule was water molecule in the unit cell. 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^)+(0.0256P)^2^+1.2174P] 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 627 _refine_ls_number_parameters 66 _refine_ls_number_restraints 5 _refine_ls_R_factor_all 0.0182 _refine_ls_R_factor_gt 0.0176 _refine_ls_wR_factor_ref 0.0509 _refine_ls_wR_factor_gt 0.0503 _refine_ls_goodness_of_fit_ref 1.160 _refine_ls_restrained_S_all 1.156 _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 Ge1 Ge 0.5000 0.5000 0.0000 0.00404(13) Uani 1 4 d S . . P1 P 0.54731(6) 1.0000 0.19512(6) 0.00381(16) Uani 1 2 d S . . O3 O 0.63317(19) 1.0000 0.34063(18) 0.0101(4) Uani 1 2 d S . . O2 O 0.40078(18) 1.0000 0.18125(18) 0.0068(4) Uani 1 2 d S . . O1 O 0.58512(12) 0.7545(2) 0.12561(12) 0.0071(3) Uani 1 1 d . . . N1 N 0.3442(2) 0.5000 0.0665(2) 0.0055(4) Uani 1 2 d SD . . N2 N 0.7717(2) 0.5000 0.3779(2) 0.0095(5) Uani 1 2 d SD . . O4 O 1.0000 1.0000 0.5000 0.116(12) Uani 0.38(2) 4 d SP . . H5 H 0.831(3) 0.5000 0.320(3) 0.019(9) Uiso 1 2 d SD . . H3 H 0.830(3) 0.5000 0.4705(15) 0.031(11) Uiso 1 2 d SD . . H4 H 0.716(2) 0.656(3) 0.361(2) 0.020(6) Uiso 1 1 d D . . H1 H 0.345(3) 0.342(3) 0.120(2) 0.025(7) Uiso 1 1 d D . . H2 H 0.264(2) 0.5000 -0.009(2) 0.019(9) Uiso 1 2 d SD . . 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 Ge1 0.0050(2) 0.00229(19) 0.0046(2) 0.000 0.00107(13) 0.000 P1 0.0058(3) 0.0025(3) 0.0027(3) 0.000 0.0006(2) 0.000 O3 0.0138(10) 0.0104(9) 0.0041(9) 0.000 -0.0007(7) 0.000 O2 0.0078(9) 0.0047(9) 0.0091(9) 0.000 0.0043(7) 0.000 O1 0.0060(6) 0.0052(6) 0.0094(6) -0.0041(5) 0.0010(5) -0.0003(5) N1 0.0052(10) 0.0046(10) 0.0069(10) 0.000 0.0022(8) 0.000 N2 0.0113(11) 0.0111(12) 0.0057(11) 0.000 0.0017(8) 0.000 O4 0.081(14) 0.060(12) 0.25(3) 0.000 0.112(17) 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 Ge1 O1 1.8778(13) 5_665 ? Ge1 O1 1.8778(13) . ? Ge1 O1 1.8778(13) 6_565 ? Ge1 O1 1.8778(13) 2_655 ? Ge1 N1 1.968(2) 5_665 ? Ge1 N1 1.968(2) . ? P1 O3 1.5169(19) . ? P1 O2 1.525(2) . ? P1 O1 1.5566(13) . ? P1 O1 1.5566(13) 6_575 ? N1 H1 0.978(3) . ? N1 H2 0.979(3) . ? N2 H5 0.979(3) . ? N2 H3 0.979(3) . ? N2 H4 0.979(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 O1 Ge1 O1 180.00(6) 5_665 . ? O1 Ge1 O1 92.06(8) 5_665 6_565 ? O1 Ge1 O1 87.94(8) . 6_565 ? O1 Ge1 O1 87.94(8) 5_665 2_655 ? O1 Ge1 O1 92.06(8) . 2_655 ? O1 Ge1 O1 180.0 6_565 2_655 ? O1 Ge1 N1 92.76(6) 5_665 5_665 ? O1 Ge1 N1 87.24(6) . 5_665 ? O1 Ge1 N1 87.24(6) 6_565 5_665 ? O1 Ge1 N1 92.76(6) 2_655 5_665 ? O1 Ge1 N1 87.24(6) 5_665 . ? O1 Ge1 N1 92.76(6) . . ? O1 Ge1 N1 92.76(6) 6_565 . ? O1 Ge1 N1 87.24(6) 2_655 . ? N1 Ge1 N1 180.00(10) 5_665 . ? O3 P1 O2 113.79(11) . . ? O3 P1 O1 107.05(7) . . ? O2 P1 O1 110.43(6) . . ? O3 P1 O1 107.05(7) . 6_575 ? O2 P1 O1 110.43(6) . 6_575 ? O1 P1 O1 107.83(10) . 6_575 ? P1 O1 Ge1 137.84(8) . . ? Ge1 N1 H1 108.8(15) . . ? Ge1 N1 H2 111(2) . . ? H1 N1 H2 108.4(18) . . ? H5 N2 H3 105(3) . . ? H5 N2 H4 110.5(17) . . ? H3 N2 H4 111.1(18) . . ? 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 O3 P1 O1 Ge1 141.17(12) . . . . ? O2 P1 O1 Ge1 16.80(15) . . . . ? O1 P1 O1 Ge1 -103.94(12) 6_575 . . . ? O1 Ge1 O1 P1 140(100) 5_665 . . . ? O1 Ge1 O1 P1 -127.42(10) 6_565 . . . ? O1 Ge1 O1 P1 52.58(10) 2_655 . . . ? N1 Ge1 O1 P1 145.25(13) 5_665 . . . ? N1 Ge1 O1 P1 -34.75(13) . . . . ? loop_ _geom_hbond_atom_site_label_D _geom_hbond_atom_site_label_H _geom_hbond_atom_site_label_A _geom_hbond_distance_DH _geom_hbond_distance_HA _geom_hbond_distance_DA _geom_hbond_angle_DHA _geom_hbond_site_symmetry_A N2 H5 O2 0.979(3) 1.796(10) 2.755(3) 166(3) 3_545 N2 H3 O3 0.979(3) 1.874(18) 2.786(3) 154(3) 7_666 N2 H4 O3 0.979(3) 1.957(6) 2.9259(17) 170(2) . N2 H4 O1 0.979(3) 2.48(2) 3.075(2) 119.0(17) . N1 H1 O2 0.978(3) 1.898(12) 2.8135(15) 155(2) 1_545 N1 H2 O2 0.979(3) 2.107(5) 3.084(3) 176(3) 7_565 _diffrn_measured_fraction_theta_max 0.830 _diffrn_reflns_theta_full 25.00 _diffrn_measured_fraction_theta_full 0.992 _refine_diff_density_max 0.388 _refine_diff_density_min -0.516 _refine_diff_density_rms 0.078