# 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 'Thomas Groshens' _publ_contact_author_email THOMAS.GROSHENS@NAVY.MIL _publ_section_title ; New Hydrogen Storage Materials Exploiting the Self-Sustaining Thermal Decomposition of Guanidinium Borohydride ; loop_ _publ_author_name 'Thomas Groshens' 'Richard A Hollins' # Attachment 'Updated CCDC 705066.cif.txt' data_tg_gbh2_0m _database_code_depnum_ccdc_archive 'CCDC 705066' _audit_creation_method SHELXL-97 _chemical_name_systematic 'Guanidinium Tetrahydroborate' _chemical_name_common 'Guanidinium Tetrahydroborate' _chemical_formula_moiety 'C H6 N3, B H4' _chemical_formula_sum 'C H10 B N3' _exptl_crystal_recrystallization_method 'From Isopropanol' _chemical_melting_point ? _exptl_crystal_description 'Tetragonal Bipyrimide' _exptl_crystal_colour Colourless _diffrn_ambient_temperature 296(2) _chemical_formula_weight 74.93 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' B B 0.0013 0.0007 '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 tetragonal _symmetry_space_group_name_H-M 'I 41/a m d' _symmetry_int_tables_number 141 _symmetry_space_group_name_Hall '-I 4bd 2' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-y+1/4, x+3/4, z+1/4' 'y+1/4, -x+1/4, z+3/4' 'x, -y, -z' '-x, y+1/2, -z' '-x, -y+1/2, z' 'y+1/4, x+3/4, -z+1/4' '-y+1/4, -x+1/4, -z+3/4' 'x+1/2, y+1/2, z+1/2' '-y+3/4, x+5/4, z+3/4' 'y+3/4, -x+3/4, z+5/4' 'x+1/2, -y+1/2, -z+1/2' '-x+1/2, y+1, -z+1/2' '-x+1/2, -y+1, z+1/2' 'y+3/4, x+5/4, -z+3/4' '-y+3/4, -x+3/4, -z+5/4' '-x, -y, -z' 'y-1/4, -x-3/4, -z-1/4' '-y-1/4, x-1/4, -z-3/4' '-x, y, z' 'x, -y-1/2, z' 'x, y-1/2, -z' '-y-1/4, -x-3/4, z-1/4' 'y-1/4, x-1/4, z-3/4' '-x+1/2, -y+1/2, -z+1/2' 'y+1/4, -x-1/4, -z+1/4' '-y+1/4, x+1/4, -z-1/4' '-x+1/2, y+1/2, z+1/2' 'x+1/2, -y, z+1/2' 'x+1/2, y, -z+1/2' '-y+1/4, -x-1/4, z+1/4' 'y+1/4, x+1/4, z-1/4' _cell_length_a 6.7433(8) _cell_length_b 6.7433(8) _cell_length_c 24.195(3) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 1100.2(2) _cell_formula_units_Z 8 _cell_measurement_temperature 296(2) _cell_measurement_reflns_used 4900 _cell_measurement_theta_min 3.136 _cell_measurement_theta_max 24.435 _exptl_crystal_size_max 0.31 _exptl_crystal_size_mid 0.20 _exptl_crystal_size_min 0.18 _exptl_crystal_density_diffrn 0.905 #Calc. density is consistant with similar high percent hydrogen atom compounds _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 336 _exptl_absorpt_coefficient_mu 0.060 _exptl_absorpt_correction_type empirical _exptl_absorpt_correction_T_min 0.9816 _exptl_absorpt_correction_T_max 0.9890 _exptl_absorpt_process_details multiscan _exptl_special_details ; ? ; _diffrn_radiation_probe ? _diffrn_radiation_type MoK\a _diffrn_radiation_wavelength 0.71073 _diffrn_source 'fine-focus sealed tube' _diffrn_radiation_monochromator graphite _diffrn_measurement_device_type 'Bruker SMART APEXII' _diffrn_measurement_method CCD _diffrn_detector_area_resol_mean ? _diffrn_reflns_number 4900 _diffrn_reflns_av_R_equivalents 0.0179 _diffrn_reflns_av_sigmaI/netI 0.0078 _diffrn_reflns_limit_h_min -8 _diffrn_reflns_limit_h_max 8 _diffrn_reflns_limit_k_min -8 _diffrn_reflns_limit_k_max 8 _diffrn_reflns_limit_l_min -28 _diffrn_reflns_limit_l_max 28 _diffrn_reflns_theta_min 3.14 _diffrn_reflns_theta_max 25.00 _reflns_number_total 287 _reflns_number_gt 235 _reflns_threshold_expression >2sigma(I) _computing_data_collection ? _computing_cell_refinement 'Bruker SHELXTL Software Package' _computing_data_reduction ? _computing_structure_solution 'SHELXS-97 (Sheldrick, 2008)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 2008)' _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^)+(0.0906P)^2^+0.1181P] 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 0.0180(70) _refine_ls_number_reflns 287 _refine_ls_number_parameters 28 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0597 _refine_ls_R_factor_gt 0.0545 _refine_ls_wR_factor_ref 0.1559 _refine_ls_wR_factor_gt 0.1461 _refine_ls_goodness_of_fit_ref 1.180 _refine_ls_restrained_S_all 1.180 _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 B1 B 0.5000 0.7500 0.07976(16) 0.1080(16) Uani 1 4 d S . . N1 N 0.8315(2) 0.7500 0.96431(7) 0.0919(8) Uani 1 2 d S . . H2 H 0.7211 0.7500 0.9821 0.110 Uiso 1 2 calc SR . . H1 H 0.8315 0.7500 0.9288 0.110 Uiso 1 2 calc SR . . N2 N 1.0000 0.7500 1.04534(10) 0.0883(9) Uani 1 4 d S . . C1 C 1.0000 0.7500 0.99142(11) 0.0694(9) Uani 1 4 d S . . H5 H 0.368(5) 0.7500 0.1041(15) 0.166(12) Uiso 1 2 d S . . H4 H 0.5000 0.656(5) 0.0412(17) 0.195(16) Uiso 1 2 d S . . H3 H 1.109(3) 0.7500 1.0587(11) 0.102(8) Uiso 1 2 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 B1 0.0686(19) 0.192(5) 0.0637(18) 0.000 0.000 0.000 N1 0.0761(12) 0.1160(15) 0.0836(12) 0.000 -0.0062(7) 0.000 N2 0.0737(18) 0.118(2) 0.0732(16) 0.000 0.000 0.000 C1 0.0670(14) 0.0644(15) 0.0769(17) 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 B1 H5 1.07(3) . ? B1 H4 1.13(4) . ? N1 H2 0.8600 . ? N1 H1 0.8600 . ? N2 C1 1.305(4) . ? N2 H3 0.80(2) . ? C1 N1 1.312(2) 20_755 ? 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 H5 B1 H4 117.2(15) . . ? C1 N1 H2 120.0 . . ? C1 N1 H1 120.0 . . ? H2 N1 H1 120.0 . . ? C1 N2 H3 113.8(19) . . ? N2 C1 N1 120.00(12) . 20_755 ? N1 C1 N1 120.0(2) . 20_755 ? _diffrn_measured_fraction_theta_max 1.000 _diffrn_reflns_theta_full 25.00 _diffrn_measured_fraction_theta_full 1.000 _refine_diff_density_max 0.165 _refine_diff_density_min -0.174 _refine_diff_density_rms 0.046