# Electronic Supplementary Material (ESI) for Dalton Transactions # This journal is © The Royal Society of Chemistry 2011 data_global _journal_name_full 'Dalton Trans.' _journal_coden_cambridge 0222 _publ_contact_author_name 'R.T. Boere' _publ_contact_author_address ; Department of Chemistry and Biochemistry University of Lethbridge Lethbridge, AB Canada T1K 3M4 ; _publ_contact_author_email boere@uleth.ca _publ_contact_author_phone +1-403-329-2045 _publ_contact_author_fax +1-403-329-2057 _publ_author_address ; Department of Chemistry and Biochemistry University of Lethbridge Lethbridge, AB Canada T1K 3M4 ; loop_ _publ_author_name R.T.Boere 'Ken Wong' 'Klaus Moock' data_H2C2N4S2 _database_code_depnum_ccdc_archive 'CCDC 836600' #TrackingRef '- Dalton01.cif' _audit_creation_method SHELXL-97 _chemical_name_systematic ; 1,5,2,4,6,8-dithiatetrazocine ; _chemical_name_common 1,5,2,4,6,8-dithiatetrazocine _chemical_melting_point 393 _chemical_formula_moiety 'C2 H2 N4 S2' _chemical_formula_sum 'C2 H2 N4 S2' _chemical_formula_weight 146.20 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' S S 0.1246 0.1234 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting Orthorhombic _symmetry_space_group_name_H-M Pbca _symmetry_int_tables_number 61 _symmetry_space_group_name_Hall '-P 2ac 2ab' 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' '-x, -y, -z' 'x-1/2, y, -z-1/2' 'x, -y-1/2, z-1/2' '-x-1/2, y-1/2, z' _cell_length_a 5.979(3) _cell_length_b 7.217(3) _cell_length_c 12.281(5) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 530.0(4) _cell_formula_units_Z 4 _cell_measurement_temperature 173(2) _cell_measurement_reflns_used 2599 _cell_measurement_theta_min 3.31 _cell_measurement_theta_max 28.37 _exptl_crystal_description Plate _exptl_crystal_colour Yellow _exptl_crystal_size_max 0.20 _exptl_crystal_size_mid 0.18 _exptl_crystal_size_min 0.08 _exptl_crystal_density_diffrn 1.832 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 296 _exptl_absorpt_coefficient_mu 0.880 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_correction_T_min 0.5724 _exptl_absorpt_correction_T_max 0.7456 _exptl_absorpt_process_details ; SADABS (Bruker, 2008) ; _exptl_special_details ; A crystal coated in Paratone (TM) oil was mounted on the end of a thin glass capillary and cooled in the gas stream of the diffractometer Kryoflex device. ; loop_ _exptl_crystal_face_index_h _exptl_crystal_face_index_k _exptl_crystal_face_index_l _exptl_crystal_face_perp_dist 0.00 1.00 -1.00 0.0600 1.00 1.00 2.00 0.0600 2.00 2.00 1.00 0.0700 -2.00 -2.00 -1.00 0.0900 -1.00 -2.00 1.00 0.0800 1.00 2.00 -1.00 0.0700 -1.00 -2.00 2.00 0.0800 -2.00 1.00 0.00 0.0800 2.00 -1.00 -2.00 0.0800 -1.00 2.00 1.00 0.0600 0.00 -1.00 0.00 0.0900 0.00 1.00 0.00 0.0600 0.00 0.00 1.00 0.0300 0.00 0.00 -1.00 0.0300 _diffrn_ambient_temperature 173(2) _diffrn_radiation_probe x-ray _diffrn_radiation_type MoK\a _diffrn_radiation_wavelength 0.71073 _diffrn_source 'fine-focus sealed tube' _diffrn_source_type 'Bruker D8' _diffrn_radiation_monochromator graphite _diffrn_measurement_device_type ; Bruker ApexII CCD area-detector diffractometer ; _diffrn_measurement_method 'phi and omega scans' _diffrn_reflns_number 5237 _diffrn_reflns_av_R_equivalents 0.0551 _diffrn_reflns_av_sigmaI/netI 0.0295 _diffrn_reflns_limit_h_min -7 _diffrn_reflns_limit_h_max 7 _diffrn_reflns_limit_k_min -9 _diffrn_reflns_limit_k_max 9 _diffrn_reflns_limit_l_min -15 _diffrn_reflns_limit_l_max 15 _diffrn_reflns_theta_min 3.32 _diffrn_reflns_theta_max 27.54 _reflns_number_total 609 _reflns_number_gt 505 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'APEX2 (Bruker, 2006)' _computing_cell_refinement 'SAINT-Plus (Bruker, 2006)' _computing_data_reduction SAINT-Plus _computing_structure_solution 'SHELXS (Sheldrick, 2008)' # if use Dual Space, write: 'SHELXD (Sheldrick, 2008)' _computing_structure_refinement 'SHELXTL (Sheldrick, 2008)' _computing_molecular_graphics 'Mercury (Macrae et al., 2006)' _computing_publication_material 'publCIF (Westrip, 2007)' # Bruker (2008). APEX2, SAINT-Plus and SADABS. Bruker AXS Inc., Madison # Wisconsin, USA. # Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122. # Macrae, D. F., Edgington, P. R., McCabe, P., Pidcock, E., Shields, G. P., # Taylor, R., Towler, M. & van de Streek, J. (2006). J. Appl. Cryst. 39, # 453-457. # Westrip, S. J. (2009). publCIF. In preparation. _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^)+(0.0628P)^2^+0.1620P] 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_number_reflns 609 _refine_ls_number_parameters 50 _refine_ls_number_restraints 1 _refine_ls_R_factor_all 0.0481 _refine_ls_R_factor_gt 0.0389 _refine_ls_wR_factor_ref 0.1117 _refine_ls_wR_factor_gt 0.1042 _refine_ls_goodness_of_fit_ref 1.109 _refine_ls_restrained_S_all 1.109 _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 S1 S 0.1969(6) 0.3961(5) -0.1058(3) 0.0320(4) Uani 0.75 1 d P A 1 N1 N -0.0137(14) 0.5047(16) -0.1518(8) 0.0301(11) Uani 0.75 1 d P . 1 N2 N 0.2612(7) 0.3608(5) 0.0165(2) 0.0305(7) Uani 0.75 1 d P A 1 C1 C 0.177(3) 0.406(3) 0.1105(19) 0.0321(9) Uani 0.75 1 d P . 1 H1 H 0.2664 0.3547 0.1670 0.039 Uiso 0.75 1 calc PR . 1 S2 S 0.200(2) 0.3989(19) 0.1099(14) 0.0321(9) Uani 0.25 1 d P . 2 N3 N 0.024(5) 0.494(5) -0.141(3) 0.0301(11) Uani 0.25 1 d PD . 2 N4 N 0.249(3) 0.376(2) -0.0163(10) 0.0305(7) Uani 0.25 1 d PD B 2 C2 C 0.180(8) 0.404(7) -0.108(4) 0.0320(4) Uani 0.25 1 d PD B 2 H2 H 0.2651 0.3450 -0.1635 0.038 Uiso 0.25 1 calc PR B 2 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 S1 0.0290(8) 0.0332(6) 0.0337(5) -0.0010(3) 0.0083(4) 0.0041(5) N1 0.034(3) 0.0327(17) 0.024(2) 0.0016(14) -0.0062(17) -0.002(2) N2 0.0242(10) 0.0307(12) 0.037(2) 0.0091(14) -0.0073(16) 0.0033(9) C1 0.027(3) 0.0338(10) 0.0357(7) 0.0022(7) -0.0119(15) 0.0039(13) S2 0.027(3) 0.0338(10) 0.0357(7) 0.0022(7) -0.0119(15) 0.0039(13) N3 0.034(3) 0.0327(17) 0.024(2) 0.0016(14) -0.0062(17) -0.002(2) N4 0.0242(10) 0.0307(12) 0.037(2) 0.0091(14) -0.0073(16) 0.0033(9) C2 0.0290(8) 0.0332(6) 0.0337(5) -0.0010(3) 0.0083(4) 0.0041(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 S1 N2 1.571(4) . ? S1 N1 1.588(6) . ? N1 C1 1.28(2) 5_565 ? N2 C1 1.30(2) . ? C1 H1 0.9500 . ? S2 N4 1.59(2) . ? S2 N3 1.59(4) 5_565 ? N3 C2 1.21(3) . ? N4 C2 1.22(3) . ? C2 H2 0.9500 . ? 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 S1 N1 127.9(6) . . ? C1 N1 S1 135.7(13) 5_565 . ? C1 N2 S1 135.6(10) . . ? N1 C1 N2 141(2) 5_565 . ? N1 C1 H1 109.6 5_565 . ? N2 C1 H1 109.6 . . ? N4 S2 N3 116.2(16) . 5_565 ? C2 N3 S2 146(4) . 5_565 ? C2 N4 S2 146(3) . . ? N3 C2 N4 131(6) . . ? N3 C2 H2 114.3 . . ? N4 C2 H2 114.3 . . ? 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 N2 S1 N1 C1 3(2) . . . 5_565 ? N1 S1 N2 C1 -1.3(13) . . . . ? S1 N2 C1 N1 -1(3) . . . 5_565 ? N3 S2 N4 C2 -3(5) 5_565 . . . ? S2 N3 C2 N4 -12(12) 5_565 . . . ? S2 N4 C2 N3 9(9) . . . . ? _diffrn_measured_fraction_theta_max 0.998 _diffrn_reflns_theta_full 25.25 _diffrn_measured_fraction_theta_full 1.000 _refine_diff_density_max 0.440 _refine_diff_density_min -0.337 _refine_diff_density_rms 0.087 _iucr_refine_instruction_details ; TITL C2H2N4S2 in Pbca CELL 0.71073 5.9794 7.2174 12.2812 90.000 90.000 90.000 ZERR 4.00 0.0026 0.0032 0.0054 0.000 0.000 0.000 LATT 1 SYMM 0.5-X, -Y, 0.5+Z SYMM -X, 0.5+Y, 0.5-Z SYMM 0.5+X, 0.5-Y, -Z SFAC C H N S UNIT 8 8 16 8 SIZE 0.08 0.18 0.20 TEMP -100 EADP S1 C2 EADP S2 C1 SADI 0.01 N3 C2 N4 C2 EADP N1 N3 EADP N2 N4 L.S. 12 MPLA 5 S1 N1 N2 C1 H1 BOND $H ACTA 50.5 CONF WGHT 0.062800 0.162000 FVAR 0.23172 PART 1 S1 4 0.196948 0.396064 -0.105848 10.75000 0.02900 0.03323 = 0.03372 -0.00103 0.00834 0.00412 N1 3 -0.013697 0.504736 -0.151806 10.75000 0.03412 0.03266 = 0.02354 0.00160 -0.00620 -0.00198 N2 3 0.261163 0.360842 0.016457 10.75000 0.02421 0.03066 = 0.03674 0.00911 -0.00728 0.00328 C1 1 0.176956 0.405559 0.110454 10.75000 0.02680 0.03380 = 0.03572 0.00224 -0.01195 0.00386 AFIX 43 H1 2 0.266359 0.354743 0.166997 10.75000 -1.20000 AFIX 0 PART 2 S2 4 0.199945 0.398880 0.109931 10.25000 0.02680 0.03380 = 0.03572 0.00224 -0.01195 0.00386 N3 3 0.023543 0.493983 -0.141451 10.25000 0.03412 0.03266 = 0.02354 0.00160 -0.00620 -0.00198 N4 3 0.248559 0.376179 -0.016326 10.25000 0.02421 0.03066 = 0.03674 0.00911 -0.00728 0.00328 C2 1 0.180324 0.404142 -0.108068 10.25000 0.02900 0.03323 = 0.03372 -0.00103 0.00834 0.00412 AFIX 43 H2 2 0.265058 0.344987 -0.163504 10.25000 -1.20000 PART 0 HKLF 4 END ; data_S4N4 _database_code_depnum_ccdc_archive 'CCDC 836601' #TrackingRef '- Dalton01.cif' # Results very similar to the re-determination at 100 K reported by # W. Scherer e.a., Chemm. Commun. (2000), 635. _audit_creation_method SHELXL-97 _chemical_name_systematic ; tetranitrogen tetrasulfide ; _chemical_name_common 'tetranitrogen tetrasulfide' _chemical_melting_point ? _chemical_formula_moiety 'N4 S4' _chemical_formula_sum 'N4 S4' _chemical_formula_weight 184.28 loop_ _atom_type_symbol _atom_type_description _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source N N 0.0061 0.0033 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' S S 0.1246 0.1234 '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)/n _symmetry_int_tables_number 14 _symmetry_space_group_name_Hall -P2yn loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x+1/2, y+1/2, -z+1/2' '-x, -y, -z' 'x-1/2, -y-1/2, z-1/2' _cell_length_a 8.647(3) _cell_length_b 7.101(3) _cell_length_c 8.732(3) _cell_angle_alpha 90.00 _cell_angle_beta 93.402(4) _cell_angle_gamma 90.00 _cell_volume 535.2(3) _cell_formula_units_Z 4 _cell_measurement_temperature 173(2) _cell_measurement_reflns_used 2555 _cell_measurement_theta_min 3.22 _cell_measurement_theta_max 27.44 _exptl_crystal_recrystallization_method 'Slow cooling' _diffrn_ambient_pressure 101 _exptl_crystal_description Needle _exptl_crystal_colour Yellow _exptl_crystal_size_max 0.287 _exptl_crystal_size_mid 0.095 _exptl_crystal_size_min 0.030 _exptl_crystal_density_diffrn 2.287 _exptl_crystal_F_000 368 _exptl_absorpt_coefficient_mu 1.649 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_correction_T_min 0.610 _exptl_absorpt_correction_T_max 0.7455 _exptl_absorpt_process_details ; SADABS (Bruker, 2006) ; _exptl_special_details ; A crystal coated in Paratone (TM) oil was mounted on the end of a thin glass capillary and cooled in the gas stream of the diffractometer Kryoflex device. ; _diffrn_ambient_temperature 173(2) _diffrn_radiation_probe x-ray _diffrn_radiation_type MoK\a _diffrn_radiation_wavelength 0.71073 _diffrn_source 'fine-focus sealed tube' _diffrn_source_type 'Bruker D8' _diffrn_radiation_monochromator graphite _diffrn_measurement_device_type ; Bruker ApexII CCD area-detector diffractometer ; _diffrn_measurement_method 'phi and omega scans' _diffrn_reflns_number 5966 _diffrn_reflns_av_R_equivalents 0.0561 _diffrn_reflns_av_sigmaI/netI 0.0517 _diffrn_reflns_limit_h_min -11 _diffrn_reflns_limit_h_max 11 _diffrn_reflns_limit_k_min -9 _diffrn_reflns_limit_k_max 9 _diffrn_reflns_limit_l_min -11 _diffrn_reflns_limit_l_max 11 _diffrn_reflns_theta_min 3.22 _diffrn_reflns_theta_max 27.48 _reflns_number_total 1228 _reflns_number_gt 958 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'APEX2 (Bruker, 2006)' _computing_cell_refinement 'SAINT-Plus (Bruker, 2006)' _computing_data_reduction SAINT-Plus _computing_structure_solution 'SHELXS (Sheldrick, 2008)' # if use Dual Space, write: 'SHELXD (Sheldrick, 2008)' _computing_structure_refinement 'SHELXTL (Sheldrick, 2008)' _computing_molecular_graphics 'Mercury (Macrae et al., 2006)' _computing_publication_material 'publCIF (Westrip, 2007)' # Bruker (2006). APEX2, SAINT-Plus and SADABS. Bruker AXS Inc., Madison # Wisconsin, USA. # Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122. # Macrae, D. F., Edgington, P. R., McCabe, P., Pidcock, E., Shields, G. P., # Taylor, R., Towler, M. & van de Streek, J. (2006). J. Appl. Cryst. 39, # 453-457. # Westrip, S. P. (2010). J. Appl. Cryst. 43, 920-925. _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^)+(0.0241P)^2^+0.0000P] where P=(Fo^2^+2Fc^2^)/3' _atom_sites_solution_primary direct _atom_sites_solution_secondary difmap _refine_ls_number_reflns 1228 _refine_ls_number_parameters 73 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0450 _refine_ls_R_factor_gt 0.0299 _refine_ls_wR_factor_ref 0.0611 _refine_ls_wR_factor_gt 0.0580 _refine_ls_goodness_of_fit_ref 0.941 _refine_ls_restrained_S_all 0.941 _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 S1 S 0.59822(8) 0.20860(10) 1.15140(8) 0.02104(18) Uani 1 1 d . . . S3 S 0.55930(8) 0.29842(10) 0.85055(8) 0.02218(18) Uani 1 1 d . . . S2 S 0.77366(8) 0.04704(10) 0.95985(8) 0.02674(19) Uani 1 1 d . . . S4 S 0.80358(8) 0.42187(10) 1.00614(8) 0.02741(19) Uani 1 1 d . . . N1 N 0.7178(3) 0.3838(3) 1.1648(2) 0.0249(6) Uani 1 1 d . . . N2 N 0.8921(3) 0.2242(3) 0.9741(3) 0.0307(6) Uani 1 1 d . . . N3 N 0.6494(3) 0.1043(3) 0.8190(2) 0.0249(6) Uani 1 1 d . . . N4 N 0.4759(3) 0.2631(3) 1.0097(2) 0.0213(5) 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 S1 0.0246(4) 0.0226(4) 0.0160(3) 0.0031(3) 0.0011(3) -0.0014(3) S3 0.0267(4) 0.0228(4) 0.0167(4) 0.0029(3) -0.0010(3) -0.0002(3) S2 0.0250(4) 0.0276(4) 0.0277(4) -0.0014(3) 0.0019(3) 0.0055(3) S4 0.0280(4) 0.0296(4) 0.0246(4) 0.0000(3) 0.0010(3) -0.0123(3) N1 0.0317(14) 0.0257(13) 0.0169(12) -0.0016(10) -0.0010(10) -0.0076(11) N2 0.0183(13) 0.0408(16) 0.0333(15) 0.0009(12) 0.0045(11) -0.0025(11) N3 0.0314(14) 0.0233(13) 0.0197(12) -0.0056(10) -0.0002(11) 0.0013(11) N4 0.0201(12) 0.0218(13) 0.0222(13) 0.0032(10) 0.0025(10) 0.0000(10) _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 S1 N1 1.617(2) . ? S1 N4 1.626(2) . ? S3 N3 1.615(2) . ? S3 N4 1.623(2) . ? S2 N2 1.622(2) . ? S2 N3 1.636(2) . ? S4 N2 1.631(3) . ? S4 N1 1.632(2) . ? 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 N1 S1 N4 104.83(12) . . ? N3 S3 N4 104.91(12) . . ? N2 S2 N3 104.39(13) . . ? N2 S4 N1 104.18(12) . . ? S1 N1 S4 112.76(13) . . ? S2 N2 S4 112.31(14) . . ? S3 N3 S2 112.71(13) . . ? S3 N4 S1 112.72(14) . . ? 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 N4 S1 N1 S4 -57.71(16) . . . . ? N2 S4 N1 S1 -58.69(17) . . . . ? N3 S2 N2 S4 58.11(17) . . . . ? N1 S4 N2 S2 58.16(17) . . . . ? N4 S3 N3 S2 -57.74(16) . . . . ? N2 S2 N3 S3 -58.85(17) . . . . ? N3 S3 N4 S1 58.07(15) . . . . ? N1 S1 N4 S3 58.14(16) . . . . ? _diffrn_measured_fraction_theta_max 0.997 _diffrn_reflns_theta_full 25.25 _diffrn_measured_fraction_theta_full 0.999 _refine_diff_density_max 0.333 _refine_diff_density_min -0.394 _refine_diff_density_rms 0.081 _iucr_refine_instruction_details ; TITL S4N4 from H-8MR synthesis in P2(1)/n CELL 0.71073 8.6469 7.1006 8.7323 90.000 93.402 90.000 ZERR 4.00 0.0031 0.0025 0.0031 0.000 0.004 0.000 LATT 1 SYMM 0.5-X, 0.5+Y, 0.5-Z SFAC N S UNIT 16 16 L.S. 18 BOND CONF ACTA 50.5 MPLA 4 S1 > S4 MPLA 4 N1 > N4 FMAP 2 PLAN 5 TEMP -100.000 WGHT 0.024100 FVAR 0.57262 S1 2 0.598220 0.208597 1.151404 11.00000 0.02455 0.02259 = 0.01598 0.00310 0.00114 -0.00142 S3 2 0.559298 0.298420 0.850554 11.00000 0.02673 0.02284 = 0.01670 0.00294 -0.00095 -0.00020 S2 2 0.773662 0.047040 0.959846 11.00000 0.02502 0.02755 = 0.02770 -0.00145 0.00194 0.00550 S4 2 0.803575 0.421865 1.006142 11.00000 0.02804 0.02957 = 0.02455 0.00003 0.00104 -0.01233 N1 1 0.717775 0.383812 1.164764 11.00000 0.03173 0.02573 = 0.01690 -0.00162 -0.00098 -0.00757 N2 1 0.892119 0.224151 0.974051 11.00000 0.01827 0.04081 = 0.03331 0.00088 0.00446 -0.00245 N3 1 0.649352 0.104298 0.819049 11.00000 0.03143 0.02327 = 0.01967 -0.00564 -0.00019 0.00130 N4 1 0.475881 0.263088 1.009706 11.00000 0.02005 0.02182 = 0.02223 0.00324 0.00249 -0.00002 HKLF 4 END ;