# Supplementary Material (ESI) for Chemical Communications
# This journal is © The Royal Society of Chemistry 2006


data_global
_journal_name_full               Chem.Commun.

_journal_coden_Cambridge         0182

_publ_contact_author_name        'Judith A. K. Howard'
_publ_contact_author_address     
;
Department of Chemistry
Durham University
South Rd
Durham
DH1 3LE
UNITED KINGDOM
;

_publ_contact_author_email       J.A.K.HOWARD@DUR.AC.UK

_publ_section_title              
;
Determination of the Hydrogen Absorption Sites in
Zn4O(1,4-benzenedicarboxylate) by Single Crystal Neutron Diffraction
;
loop_
_publ_author_name
'Judith A. K. Howard'
'Garry J. McIntyre'
'Jesse L. C. Rowsell'
'Elinor Spencer'
'Omar Yaghi'

# Attachment 'CIF2.txt'

data_5k
_database_code_depnum_ccdc_archive 'CCDC 282407'

_audit_creation_method           SHELXL-97
_chemical_name_systematic        
;
Hydrogen-Loaded Zn4O(1,4-Benzenedicarboxylate)
;
_chemical_name_common            
'Hydrogen-Loaded Zn4O(1,4-Benzenedicarboxylate)'
_chemical_melting_point          ?
_chemical_formula_moiety         'C24 H12 O13 Zn4, 4(H2), 4(H)'
_chemical_formula_sum            'C24 H23.94 O13 Zn4'
_chemical_formula_weight         779.94

loop_
_atom_type_symbol
_atom_type_description
_atom_type_scat_dispersion_real
_atom_type_scat_dispersion_imag
_atom_type_scat_source
C C 0.0000 0.0000 '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 0.0000 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'
Zn Zn 0.0000 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'

_symmetry_cell_setting           Cubic
_symmetry_space_group_name_H-M   Fm-3m
_symmetry_space_group_name_Hall  '-F 4 2 3'

loop_
_symmetry_equiv_pos_as_xyz
'x, y, z'
'-x, -y, z'
'-x, y, -z'
'x, -y, -z'
'z, x, y'
'z, -x, -y'
'-z, -x, y'
'-z, x, -y'
'y, z, x'
'-y, z, -x'
'y, -z, -x'
'-y, -z, x'
'y, x, -z'
'-y, -x, -z'
'y, -x, z'
'-y, x, z'
'x, z, -y'
'-x, z, y'
'-x, -z, -y'
'x, -z, y'
'z, y, -x'
'z, -y, x'
'-z, y, x'
'-z, -y, -x'
'x, y+1/2, z+1/2'
'-x, -y+1/2, z+1/2'
'-x, y+1/2, -z+1/2'
'x, -y+1/2, -z+1/2'
'z, x+1/2, y+1/2'
'z, -x+1/2, -y+1/2'
'-z, -x+1/2, y+1/2'
'-z, x+1/2, -y+1/2'
'y, z+1/2, x+1/2'
'-y, z+1/2, -x+1/2'
'y, -z+1/2, -x+1/2'
'-y, -z+1/2, x+1/2'
'y, x+1/2, -z+1/2'
'-y, -x+1/2, -z+1/2'
'y, -x+1/2, z+1/2'
'-y, x+1/2, z+1/2'
'x, z+1/2, -y+1/2'
'-x, z+1/2, y+1/2'
'-x, -z+1/2, -y+1/2'
'x, -z+1/2, y+1/2'
'z, y+1/2, -x+1/2'
'z, -y+1/2, x+1/2'
'-z, y+1/2, x+1/2'
'-z, -y+1/2, -x+1/2'
'x+1/2, y, z+1/2'
'-x+1/2, -y, z+1/2'
'-x+1/2, y, -z+1/2'
'x+1/2, -y, -z+1/2'
'z+1/2, x, y+1/2'
'z+1/2, -x, -y+1/2'
'-z+1/2, -x, y+1/2'
'-z+1/2, x, -y+1/2'
'y+1/2, z, x+1/2'
'-y+1/2, z, -x+1/2'
'y+1/2, -z, -x+1/2'
'-y+1/2, -z, x+1/2'
'y+1/2, x, -z+1/2'
'-y+1/2, -x, -z+1/2'
'y+1/2, -x, z+1/2'
'-y+1/2, x, z+1/2'
'x+1/2, z, -y+1/2'
'-x+1/2, z, y+1/2'
'-x+1/2, -z, -y+1/2'
'x+1/2, -z, y+1/2'
'z+1/2, y, -x+1/2'
'z+1/2, -y, x+1/2'
'-z+1/2, y, x+1/2'
'-z+1/2, -y, -x+1/2'
'x+1/2, y+1/2, z'
'-x+1/2, -y+1/2, z'
'-x+1/2, y+1/2, -z'
'x+1/2, -y+1/2, -z'
'z+1/2, x+1/2, y'
'z+1/2, -x+1/2, -y'
'-z+1/2, -x+1/2, y'
'-z+1/2, x+1/2, -y'
'y+1/2, z+1/2, x'
'-y+1/2, z+1/2, -x'
'y+1/2, -z+1/2, -x'
'-y+1/2, -z+1/2, x'
'y+1/2, x+1/2, -z'
'-y+1/2, -x+1/2, -z'
'y+1/2, -x+1/2, z'
'-y+1/2, x+1/2, z'
'x+1/2, z+1/2, -y'
'-x+1/2, z+1/2, y'
'-x+1/2, -z+1/2, -y'
'x+1/2, -z+1/2, y'
'z+1/2, y+1/2, -x'
'z+1/2, -y+1/2, x'
'-z+1/2, y+1/2, x'
'-z+1/2, -y+1/2, -x'
'-x, -y, -z'
'x, y, -z'
'x, -y, z'
'-x, y, z'
'-z, -x, -y'
'-z, x, y'
'z, x, -y'
'z, -x, y'
'-y, -z, -x'
'y, -z, x'
'-y, z, x'
'y, z, -x'
'-y, -x, z'
'y, x, z'
'-y, x, -z'
'y, -x, -z'
'-x, -z, y'
'x, -z, -y'
'x, z, y'
'-x, z, -y'
'-z, -y, x'
'-z, y, -x'
'z, -y, -x'
'z, y, x'
'-x, -y+1/2, -z+1/2'
'x, y+1/2, -z+1/2'
'x, -y+1/2, z+1/2'
'-x, y+1/2, z+1/2'
'-z, -x+1/2, -y+1/2'
'-z, x+1/2, y+1/2'
'z, x+1/2, -y+1/2'
'z, -x+1/2, y+1/2'
'-y, -z+1/2, -x+1/2'
'y, -z+1/2, x+1/2'
'-y, z+1/2, x+1/2'
'y, z+1/2, -x+1/2'
'-y, -x+1/2, z+1/2'
'y, x+1/2, z+1/2'
'-y, x+1/2, -z+1/2'
'y, -x+1/2, -z+1/2'
'-x, -z+1/2, y+1/2'
'x, -z+1/2, -y+1/2'
'x, z+1/2, y+1/2'
'-x, z+1/2, -y+1/2'
'-z, -y+1/2, x+1/2'
'-z, y+1/2, -x+1/2'
'z, -y+1/2, -x+1/2'
'z, y+1/2, x+1/2'
'-x+1/2, -y, -z+1/2'
'x+1/2, y, -z+1/2'
'x+1/2, -y, z+1/2'
'-x+1/2, y, z+1/2'
'-z+1/2, -x, -y+1/2'
'-z+1/2, x, y+1/2'
'z+1/2, x, -y+1/2'
'z+1/2, -x, y+1/2'
'-y+1/2, -z, -x+1/2'
'y+1/2, -z, x+1/2'
'-y+1/2, z, x+1/2'
'y+1/2, z, -x+1/2'
'-y+1/2, -x, z+1/2'
'y+1/2, x, z+1/2'
'-y+1/2, x, -z+1/2'
'y+1/2, -x, -z+1/2'
'-x+1/2, -z, y+1/2'
'x+1/2, -z, -y+1/2'
'x+1/2, z, y+1/2'
'-x+1/2, z, -y+1/2'
'-z+1/2, -y, x+1/2'
'-z+1/2, y, -x+1/2'
'z+1/2, -y, -x+1/2'
'z+1/2, y, x+1/2'
'-x+1/2, -y+1/2, -z'
'x+1/2, y+1/2, -z'
'x+1/2, -y+1/2, z'
'-x+1/2, y+1/2, z'
'-z+1/2, -x+1/2, -y'
'-z+1/2, x+1/2, y'
'z+1/2, x+1/2, -y'
'z+1/2, -x+1/2, y'
'-y+1/2, -z+1/2, -x'
'y+1/2, -z+1/2, x'
'-y+1/2, z+1/2, x'
'y+1/2, z+1/2, -x'
'-y+1/2, -x+1/2, z'
'y+1/2, x+1/2, z'
'-y+1/2, x+1/2, -z'
'y+1/2, -x+1/2, -z'
'-x+1/2, -z+1/2, y'
'x+1/2, -z+1/2, -y'
'x+1/2, z+1/2, y'
'-x+1/2, z+1/2, -y'
'-z+1/2, -y+1/2, x'
'-z+1/2, y+1/2, -x'
'z+1/2, -y+1/2, -x'
'z+1/2, y+1/2, x'

_cell_length_a                   25.8821(5)
_cell_length_b                   25.8821(5)
_cell_length_c                   25.8821(5)
_cell_angle_alpha                90.00
_cell_angle_beta                 90.00
_cell_angle_gamma                90.00
_cell_volume                     17338.0(6)
_cell_formula_units_Z            8
_cell_measurement_temperature    5(2)
_cell_measurement_reflns_used    ?
_cell_measurement_theta_min      ?
_cell_measurement_theta_max      ?

_exptl_crystal_description       Block
_exptl_crystal_colour            Colourless
_exptl_crystal_size_max          0.6
_exptl_crystal_size_mid          0.6
_exptl_crystal_size_min          0.4
_exptl_crystal_density_meas      'Not measured'
_exptl_crystal_density_diffrn    0.598
_exptl_crystal_density_method    'not measured'
_exptl_crystal_F_000             1345
_exptl_absorpt_coefficient_mu    0.000
_exptl_absorpt_correction_type   None
_exptl_absorpt_correction_T_min  ?
_exptl_absorpt_correction_T_max  ?
_exptl_absorpt_process_details   ?

_exptl_special_details           
;
?
;

_diffrn_ambient_temperature      5(2)
_diffrn_radiation_wavelength     0.85-3.5
_diffrn_radiation_type           Neutron
_diffrn_radiation_source         'ILL high-flux reactor'
_diffrn_radiation_monochromator  graphite
_diffrn_measurement_device_type  'VIVALDI Neutron Laue Diffractometer'
_diffrn_measurement_method       'Laue method'
_diffrn_detector_area_resol_mean ?
_diffrn_standards_number         0
_diffrn_standards_interval_count 0
_diffrn_standards_interval_time  0
_diffrn_standards_decay_%        0
_diffrn_reflns_number            12351
_diffrn_reflns_av_R_equivalents  0.3922
_diffrn_reflns_av_sigmaI/netI    0.1345
_diffrn_reflns_limit_h_min       -26
_diffrn_reflns_limit_h_max       26
_diffrn_reflns_limit_k_min       -26
_diffrn_reflns_limit_k_max       18
_diffrn_reflns_limit_l_min       -19
_diffrn_reflns_limit_l_max       19
_diffrn_reflns_theta_min         1.36
_diffrn_reflns_theta_max         21.41
_reflns_number_total             434
_reflns_number_gt                406
_reflns_threshold_expression     >2sigma(I)

_computing_data_collection       'VIVALDI Controller'
_computing_cell_refinement       'LAUEGEN (Campbell, 1998)'
_computing_data_reduction        
;
INTERGRATE & LAUENORM (Wilkinson, 1998)(Campbell, 1996)
;
_computing_structure_solution    'SHELXS-97 (Sheldrick, 1990)'
_computing_structure_refinement  'SHELXL-97 (Sheldrick, 1997)'
_computing_molecular_graphics    'OLEX (Dolomanov, 2003)'
_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.

Initially the occupancy and Uiso values for the hydrogen gas atoms were
jointly refined (after separate refinement). The H1-H2 molecule occupancy
became 105% (with approx. 10% error) and the Uiso values were large and
unrealistic. For this reason the occupancy was fixed to 100%. This gave
more realistic Uiso values for H1 and H2.

For H4 the joint refinement of the occupancy value and Uiso gave
values of 0.16(3) and 0.17(5) respectively. For consistency, the
occupany was fixed at this refined value and the Uiso refined
freely. Only a small alteration in Uiso was observed [final value
0.18(3)]
;

_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^)+(0.0002P)^2^+0.0000P] where P=(Fo^2^+2Fc^2^)/3'
_atom_sites_solution_primary     direct
_atom_sites_solution_secondary   difmap
_atom_sites_solution_hydrogens   difmap
_refine_ls_hydrogen_treatment    refall
_refine_ls_extinction_method     none
_refine_ls_extinction_coef       'Not refined'
_refine_ls_number_reflns         434
_refine_ls_number_parameters     24
_refine_ls_number_restraints     0
_refine_ls_R_factor_all          0.2623
_refine_ls_R_factor_gt           0.2444
_refine_ls_wR_factor_ref         0.2485
_refine_ls_wR_factor_gt          0.2476
_refine_ls_goodness_of_fit_ref   3.117
_refine_ls_restrained_S_all      3.117
_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
Zn1 Zn 0.2934(3) 0.2934(3) 0.2066(3) 0.013(4) Uiso 1 6 d S . .
O1 O 0.2500 0.2500 0.2500 0.022(8) Uiso 1 24 d S . .
O2 O 0.2807(2) 0.3661(3) 0.2193(2) 0.023(3) Uiso 1 2 d S . .
C1 C 0.2500 0.3895(4) 0.2500 0.013(2) Uiso 1 4 d S . .
C2 C 0.2500 0.4452(4) 0.2500 0.014(2) Uiso 1 4 d S . .
C3 C 0.2831(2) 0.4736(3) 0.2169(2) 0.0174(19) Uiso 1 2 d S . .
H3 H 0.3077(5) 0.4522(7) 0.1923(5) 0.042(4) Uiso 1 2 d S . .
H1 H 0.3337(13) 0.3337(13) 0.3337(13) 0.088(19) Uiso 1 6 d S . .
H2 H 0.3328(15) 0.361(2) 0.3328(15) 0.05(2) Uiso 0.33 2 d SP . .
H4 H 0.3746(13) 0.3746(13) 0.1254(13) 0.18(3) Uiso 0.98 6 d SP . .

_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
O2 C1 1.275(10) . ?
C1 O2 1.275(10) 51 ?
C1 C2 1.442(16) . ?
C2 C3 1.416(8) . ?
C2 C3 1.416(8) 51 ?
C3 H3 1.06(2) . ?
C3 C3 1.369(14) 99_565 ?
C3 H3 1.06(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
O2 C1 O2 123.4(11) . 51 ?
O2 C1 C2 118.3(5) . . ?
O2 C1 C2 118.3(5) 51 . ?
C3 C2 C3 117.6(9) . 51 ?
C3 C2 C1 121.2(5) . . ?
C3 C2 C1 121.2(5) 51 . ?
H3 C3 C3 121.4(9) . 99_565 ?
H3 C3 C2 117.4(10) . . ?
C3 C3 C2 121.2(5) 99_565 . ?
H3 C3 H3 0(3) . . ?
C3 C3 H3 121.4(9) 99_565 . ?
C2 C3 H3 117.4(10) . . ?

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
O2 C1 C2 C3 0.000(1) . . . . ?
O2 C1 C2 C3 180.000(1) 51 . . . ?
O2 C1 C2 C3 180.000(1) . . . 51 ?
O2 C1 C2 C3 0.000(2) 51 . . 51 ?
C3 C2 C3 H3 180.000(3) 51 . . . ?
C1 C2 C3 H3 0.000(3) . . . . ?
C3 C2 C3 C3 0.000(2) 51 . . 99_565 ?
C1 C2 C3 C3 180.000(1) . . . 99_565 ?

_diffrn_measured_fraction_theta_max 0.781
_diffrn_reflns_theta_full        21.41
_diffrn_measured_fraction_theta_full 0.781
_refine_diff_density_max         0.983
_refine_diff_density_min         -0.593
_refine_diff_density_rms         0.130

data_30K
_database_code_depnum_ccdc_archive 'CCDC 282408'

_audit_creation_method           SHELXL-97
_chemical_name_systematic        
;
Hydrogen-Loaded Zn4O(1,4-Benzenedicarboxylate)
;
_chemical_name_common            
'Hydrogen-Loaded Zn4O(1,4-Benzenedicarboxylate)'
_chemical_melting_point          ?
_chemical_formula_moiety         'C24 H12 O13 Zn4, 4(H2)'
_chemical_formula_sum            'C24 H20 O13 Zn4'
_chemical_formula_weight         776.00

loop_
_atom_type_symbol
_atom_type_description
_atom_type_scat_dispersion_real
_atom_type_scat_dispersion_imag
_atom_type_scat_source
C C 0.0000 0.0000 '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 0.0000 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'
Zn Zn 0.0000 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'

_symmetry_cell_setting           Cubic
_symmetry_space_group_name_H-M   Fm-3m
_symmetry_space_group_name_Hall  '-F 4 2 3'

loop_
_symmetry_equiv_pos_as_xyz
'x, y, z'
'-x, -y, z'
'-x, y, -z'
'x, -y, -z'
'z, x, y'
'z, -x, -y'
'-z, -x, y'
'-z, x, -y'
'y, z, x'
'-y, z, -x'
'y, -z, -x'
'-y, -z, x'
'y, x, -z'
'-y, -x, -z'
'y, -x, z'
'-y, x, z'
'x, z, -y'
'-x, z, y'
'-x, -z, -y'
'x, -z, y'
'z, y, -x'
'z, -y, x'
'-z, y, x'
'-z, -y, -x'
'x, y+1/2, z+1/2'
'-x, -y+1/2, z+1/2'
'-x, y+1/2, -z+1/2'
'x, -y+1/2, -z+1/2'
'z, x+1/2, y+1/2'
'z, -x+1/2, -y+1/2'
'-z, -x+1/2, y+1/2'
'-z, x+1/2, -y+1/2'
'y, z+1/2, x+1/2'
'-y, z+1/2, -x+1/2'
'y, -z+1/2, -x+1/2'
'-y, -z+1/2, x+1/2'
'y, x+1/2, -z+1/2'
'-y, -x+1/2, -z+1/2'
'y, -x+1/2, z+1/2'
'-y, x+1/2, z+1/2'
'x, z+1/2, -y+1/2'
'-x, z+1/2, y+1/2'
'-x, -z+1/2, -y+1/2'
'x, -z+1/2, y+1/2'
'z, y+1/2, -x+1/2'
'z, -y+1/2, x+1/2'
'-z, y+1/2, x+1/2'
'-z, -y+1/2, -x+1/2'
'x+1/2, y, z+1/2'
'-x+1/2, -y, z+1/2'
'-x+1/2, y, -z+1/2'
'x+1/2, -y, -z+1/2'
'z+1/2, x, y+1/2'
'z+1/2, -x, -y+1/2'
'-z+1/2, -x, y+1/2'
'-z+1/2, x, -y+1/2'
'y+1/2, z, x+1/2'
'-y+1/2, z, -x+1/2'
'y+1/2, -z, -x+1/2'
'-y+1/2, -z, x+1/2'
'y+1/2, x, -z+1/2'
'-y+1/2, -x, -z+1/2'
'y+1/2, -x, z+1/2'
'-y+1/2, x, z+1/2'
'x+1/2, z, -y+1/2'
'-x+1/2, z, y+1/2'
'-x+1/2, -z, -y+1/2'
'x+1/2, -z, y+1/2'
'z+1/2, y, -x+1/2'
'z+1/2, -y, x+1/2'
'-z+1/2, y, x+1/2'
'-z+1/2, -y, -x+1/2'
'x+1/2, y+1/2, z'
'-x+1/2, -y+1/2, z'
'-x+1/2, y+1/2, -z'
'x+1/2, -y+1/2, -z'
'z+1/2, x+1/2, y'
'z+1/2, -x+1/2, -y'
'-z+1/2, -x+1/2, y'
'-z+1/2, x+1/2, -y'
'y+1/2, z+1/2, x'
'-y+1/2, z+1/2, -x'
'y+1/2, -z+1/2, -x'
'-y+1/2, -z+1/2, x'
'y+1/2, x+1/2, -z'
'-y+1/2, -x+1/2, -z'
'y+1/2, -x+1/2, z'
'-y+1/2, x+1/2, z'
'x+1/2, z+1/2, -y'
'-x+1/2, z+1/2, y'
'-x+1/2, -z+1/2, -y'
'x+1/2, -z+1/2, y'
'z+1/2, y+1/2, -x'
'z+1/2, -y+1/2, x'
'-z+1/2, y+1/2, x'
'-z+1/2, -y+1/2, -x'
'-x, -y, -z'
'x, y, -z'
'x, -y, z'
'-x, y, z'
'-z, -x, -y'
'-z, x, y'
'z, x, -y'
'z, -x, y'
'-y, -z, -x'
'y, -z, x'
'-y, z, x'
'y, z, -x'
'-y, -x, z'
'y, x, z'
'-y, x, -z'
'y, -x, -z'
'-x, -z, y'
'x, -z, -y'
'x, z, y'
'-x, z, -y'
'-z, -y, x'
'-z, y, -x'
'z, -y, -x'
'z, y, x'
'-x, -y+1/2, -z+1/2'
'x, y+1/2, -z+1/2'
'x, -y+1/2, z+1/2'
'-x, y+1/2, z+1/2'
'-z, -x+1/2, -y+1/2'
'-z, x+1/2, y+1/2'
'z, x+1/2, -y+1/2'
'z, -x+1/2, y+1/2'
'-y, -z+1/2, -x+1/2'
'y, -z+1/2, x+1/2'
'-y, z+1/2, x+1/2'
'y, z+1/2, -x+1/2'
'-y, -x+1/2, z+1/2'
'y, x+1/2, z+1/2'
'-y, x+1/2, -z+1/2'
'y, -x+1/2, -z+1/2'
'-x, -z+1/2, y+1/2'
'x, -z+1/2, -y+1/2'
'x, z+1/2, y+1/2'
'-x, z+1/2, -y+1/2'
'-z, -y+1/2, x+1/2'
'-z, y+1/2, -x+1/2'
'z, -y+1/2, -x+1/2'
'z, y+1/2, x+1/2'
'-x+1/2, -y, -z+1/2'
'x+1/2, y, -z+1/2'
'x+1/2, -y, z+1/2'
'-x+1/2, y, z+1/2'
'-z+1/2, -x, -y+1/2'
'-z+1/2, x, y+1/2'
'z+1/2, x, -y+1/2'
'z+1/2, -x, y+1/2'
'-y+1/2, -z, -x+1/2'
'y+1/2, -z, x+1/2'
'-y+1/2, z, x+1/2'
'y+1/2, z, -x+1/2'
'-y+1/2, -x, z+1/2'
'y+1/2, x, z+1/2'
'-y+1/2, x, -z+1/2'
'y+1/2, -x, -z+1/2'
'-x+1/2, -z, y+1/2'
'x+1/2, -z, -y+1/2'
'x+1/2, z, y+1/2'
'-x+1/2, z, -y+1/2'
'-z+1/2, -y, x+1/2'
'-z+1/2, y, -x+1/2'
'z+1/2, -y, -x+1/2'
'z+1/2, y, x+1/2'
'-x+1/2, -y+1/2, -z'
'x+1/2, y+1/2, -z'
'x+1/2, -y+1/2, z'
'-x+1/2, y+1/2, z'
'-z+1/2, -x+1/2, -y'
'-z+1/2, x+1/2, y'
'z+1/2, x+1/2, -y'
'z+1/2, -x+1/2, y'
'-y+1/2, -z+1/2, -x'
'y+1/2, -z+1/2, x'
'-y+1/2, z+1/2, x'
'y+1/2, z+1/2, -x'
'-y+1/2, -x+1/2, z'
'y+1/2, x+1/2, z'
'-y+1/2, x+1/2, -z'
'y+1/2, -x+1/2, -z'
'-x+1/2, -z+1/2, y'
'x+1/2, -z+1/2, -y'
'x+1/2, z+1/2, y'
'-x+1/2, z+1/2, -y'
'-z+1/2, -y+1/2, x'
'-z+1/2, y+1/2, -x'
'z+1/2, -y+1/2, -x'
'z+1/2, y+1/2, x'

_cell_length_a                   25.8821(5)
_cell_length_b                   25.8821(5)
_cell_length_c                   25.8821(5)
_cell_angle_alpha                90.00
_cell_angle_beta                 90.00
_cell_angle_gamma                90.00
_cell_volume                     17338.0(6)
_cell_formula_units_Z            8
_cell_measurement_temperature    30(2)
_cell_measurement_reflns_used    ?
_cell_measurement_theta_min      ?
_cell_measurement_theta_max      ?

_exptl_crystal_description       Block
_exptl_crystal_colour            Colourless
_exptl_crystal_size_max          0.6
_exptl_crystal_size_mid          0.6
_exptl_crystal_size_min          0.4
_exptl_crystal_density_meas      'Not measured'
_exptl_crystal_density_diffrn    0.595
_exptl_crystal_density_method    'not measured'
_exptl_crystal_F_000             1463
_exptl_absorpt_coefficient_mu    0.000
_exptl_absorpt_correction_type   ?
_exptl_absorpt_correction_T_min  ?
_exptl_absorpt_correction_T_max  ?
_exptl_absorpt_process_details   ?

_exptl_special_details           
;
?
;

_diffrn_ambient_temperature      30(2)
_diffrn_radiation_wavelength     0.85-3.5
_diffrn_radiation_type           Neutron
_diffrn_radiation_source         'ILL high-flux reactor'
_diffrn_radiation_monochromator  graphite
_diffrn_measurement_device_type  'VIVALDI Neutron Laue Diffractometer'
_diffrn_measurement_method       'Laue method'
_diffrn_detector_area_resol_mean ?
_diffrn_standards_number         0
_diffrn_standards_interval_count 0
_diffrn_standards_interval_time  0
_diffrn_standards_decay_%        0
_diffrn_reflns_number            6187
_diffrn_reflns_av_R_equivalents  0.3826
_diffrn_reflns_av_sigmaI/netI    0.1722
_diffrn_reflns_limit_h_min       -20
_diffrn_reflns_limit_h_max       26
_diffrn_reflns_limit_k_min       -26
_diffrn_reflns_limit_k_max       13
_diffrn_reflns_limit_l_min       -19
_diffrn_reflns_limit_l_max       19
_diffrn_reflns_theta_min         1.36
_diffrn_reflns_theta_max         21.17
_reflns_number_total             416
_reflns_number_gt                364
_reflns_threshold_expression     >2sigma(I)

_computing_data_collection       'VIVALDI Controller'
_computing_cell_refinement       'LAUEGEN (Campbell, 1998)'
_computing_data_reduction        
;
INTERGRATE & LAUENORM (Wilkinson, 1998)(Campbell, 1996)
;
_computing_structure_solution    'SHELXS-97 (Sheldrick, 1990)'
_computing_structure_refinement  'SHELXL-97 (Sheldrick, 1997)'
_computing_molecular_graphics    'OLEX (Dolomanov, 2003)'
_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.

Initially the occupancy and Uiso values for the hydrogen gas atoms were
jointly refined (after separate refinement). The H1-H2 molecule occupancy
became >107% (approx error of 10%) and the Uiso values were large and
unrealistic. For this reason the occupancy was fixed to 100%. This gave
more realistic Uiso values for H1 and H2.
;

_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^)+(0.0441P)^2^+0.0000P] where P=(Fo^2^+2Fc^2^)/3'
_atom_sites_solution_primary     direct
_atom_sites_solution_secondary   difmap
_atom_sites_solution_hydrogens   difmap
_refine_ls_hydrogen_treatment    refall
_refine_ls_extinction_method     none
_refine_ls_extinction_coef       'Not refined'
_refine_ls_number_reflns         416
_refine_ls_number_parameters     22
_refine_ls_number_restraints     0
_refine_ls_R_factor_all          0.2546
_refine_ls_R_factor_gt           0.2304
_refine_ls_wR_factor_ref         0.2886
_refine_ls_wR_factor_gt          0.2834
_refine_ls_goodness_of_fit_ref   2.130
_refine_ls_restrained_S_all      2.130
_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
Zn1 Zn 0.2936(3) 0.2936(3) 0.2064(3) 0.015(4) Uiso 1 6 d S . .
O1 O 0.2500 0.2500 0.2500 0.016(8) Uiso 1 24 d S . .
O2 O 0.2808(2) 0.3667(3) 0.2192(2) 0.024(3) Uiso 1 2 d S . .
C1 C 0.2500 0.3895(4) 0.2500 0.016(3) Uiso 1 4 d S . .
C2 C 0.2500 0.4457(5) 0.2500 0.016(3) Uiso 1 4 d S . .
C3 C 0.2828(2) 0.4736(3) 0.2172(2) 0.019(2) Uiso 1 2 d S . .
H3 H 0.3071(5) 0.4515(7) 0.1929(5) 0.043(5) Uiso 1 2 d S . .
H1 H 0.3323(15) 0.1677(15) 0.1677(15) 0.10(2) Uiso 1 6 d S . .
H2 H 0.3323(13) 0.1677(13) 0.140(2) 0.04(2) Uiso 0.33 2 d SP . .

_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
O2 C1 1.274(11) . ?
C1 O2 1.274(11) 51 ?
C1 C2 1.455(18) . ?
C2 C3 1.400(9) 51 ?
C2 C3 1.400(9) . ?
C3 C3 1.366(15) 99_565 ?
C3 H3 1.06(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
O2 C1 O2 124.8(12) . 51 ?
O2 C1 C2 117.6(6) . . ?
O2 C1 C2 117.6(6) 51 . ?
C3 C2 C3 118.0(11) 51 . ?
C3 C2 C1 121.0(5) 51 . ?
C3 C2 C1 121.0(5) . . ?
C3 C3 C2 121.0(5) 99_565 . ?
C3 C3 H3 122.7(9) 99_565 . ?
C2 C3 H3 116.2(11) . . ?

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
O2 C1 C2 C3 180.000(2) . . . 51 ?
O2 C1 C2 C3 0.000(2) 51 . . 51 ?
O2 C1 C2 C3 0.000(2) . . . . ?
O2 C1 C2 C3 180.000(2) 51 . . . ?
C3 C2 C3 C3 0.000(2) 51 . . 99_565 ?
C1 C2 C3 C3 180.000(1) . . . 99_565 ?

_diffrn_measured_fraction_theta_max 0.766
_diffrn_reflns_theta_full        21.17
_diffrn_measured_fraction_theta_full 0.766
_refine_diff_density_max         0.700
_refine_diff_density_min         -0.634
_refine_diff_density_rms         0.107

data_50K
_database_code_depnum_ccdc_archive 'CCDC 282409'

_audit_creation_method           SHELXL-97
_chemical_name_systematic        
;
Hydrogen-Loaded Zn4O(1,4-Benzenedicarboxylate)
;
_chemical_name_common            
'Hydrogen-Loaded Zn4O(1,4-Benzenedicarboxylate)'
_chemical_melting_point          ?
_chemical_formula_moiety         'C24 H12 O13 Zn4, 4(H)'
_chemical_formula_sum            'C24 H16 O13 Zn4'
_chemical_formula_weight         772.00

loop_
_atom_type_symbol
_atom_type_description
_atom_type_scat_dispersion_real
_atom_type_scat_dispersion_imag
_atom_type_scat_source
C C 0.0000 0.0000 '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 0.0000 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'
Zn Zn 0.0000 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'

_symmetry_cell_setting           Cubic
_symmetry_space_group_name_H-M   Fm-3m
_symmetry_space_group_name_Hall  '-F 4 2 3'

loop_
_symmetry_equiv_pos_as_xyz
'x, y, z'
'-x, -y, z'
'-x, y, -z'
'x, -y, -z'
'z, x, y'
'z, -x, -y'
'-z, -x, y'
'-z, x, -y'
'y, z, x'
'-y, z, -x'
'y, -z, -x'
'-y, -z, x'
'y, x, -z'
'-y, -x, -z'
'y, -x, z'
'-y, x, z'
'x, z, -y'
'-x, z, y'
'-x, -z, -y'
'x, -z, y'
'z, y, -x'
'z, -y, x'
'-z, y, x'
'-z, -y, -x'
'x, y+1/2, z+1/2'
'-x, -y+1/2, z+1/2'
'-x, y+1/2, -z+1/2'
'x, -y+1/2, -z+1/2'
'z, x+1/2, y+1/2'
'z, -x+1/2, -y+1/2'
'-z, -x+1/2, y+1/2'
'-z, x+1/2, -y+1/2'
'y, z+1/2, x+1/2'
'-y, z+1/2, -x+1/2'
'y, -z+1/2, -x+1/2'
'-y, -z+1/2, x+1/2'
'y, x+1/2, -z+1/2'
'-y, -x+1/2, -z+1/2'
'y, -x+1/2, z+1/2'
'-y, x+1/2, z+1/2'
'x, z+1/2, -y+1/2'
'-x, z+1/2, y+1/2'
'-x, -z+1/2, -y+1/2'
'x, -z+1/2, y+1/2'
'z, y+1/2, -x+1/2'
'z, -y+1/2, x+1/2'
'-z, y+1/2, x+1/2'
'-z, -y+1/2, -x+1/2'
'x+1/2, y, z+1/2'
'-x+1/2, -y, z+1/2'
'-x+1/2, y, -z+1/2'
'x+1/2, -y, -z+1/2'
'z+1/2, x, y+1/2'
'z+1/2, -x, -y+1/2'
'-z+1/2, -x, y+1/2'
'-z+1/2, x, -y+1/2'
'y+1/2, z, x+1/2'
'-y+1/2, z, -x+1/2'
'y+1/2, -z, -x+1/2'
'-y+1/2, -z, x+1/2'
'y+1/2, x, -z+1/2'
'-y+1/2, -x, -z+1/2'
'y+1/2, -x, z+1/2'
'-y+1/2, x, z+1/2'
'x+1/2, z, -y+1/2'
'-x+1/2, z, y+1/2'
'-x+1/2, -z, -y+1/2'
'x+1/2, -z, y+1/2'
'z+1/2, y, -x+1/2'
'z+1/2, -y, x+1/2'
'-z+1/2, y, x+1/2'
'-z+1/2, -y, -x+1/2'
'x+1/2, y+1/2, z'
'-x+1/2, -y+1/2, z'
'-x+1/2, y+1/2, -z'
'x+1/2, -y+1/2, -z'
'z+1/2, x+1/2, y'
'z+1/2, -x+1/2, -y'
'-z+1/2, -x+1/2, y'
'-z+1/2, x+1/2, -y'
'y+1/2, z+1/2, x'
'-y+1/2, z+1/2, -x'
'y+1/2, -z+1/2, -x'
'-y+1/2, -z+1/2, x'
'y+1/2, x+1/2, -z'
'-y+1/2, -x+1/2, -z'
'y+1/2, -x+1/2, z'
'-y+1/2, x+1/2, z'
'x+1/2, z+1/2, -y'
'-x+1/2, z+1/2, y'
'-x+1/2, -z+1/2, -y'
'x+1/2, -z+1/2, y'
'z+1/2, y+1/2, -x'
'z+1/2, -y+1/2, x'
'-z+1/2, y+1/2, x'
'-z+1/2, -y+1/2, -x'
'-x, -y, -z'
'x, y, -z'
'x, -y, z'
'-x, y, z'
'-z, -x, -y'
'-z, x, y'
'z, x, -y'
'z, -x, y'
'-y, -z, -x'
'y, -z, x'
'-y, z, x'
'y, z, -x'
'-y, -x, z'
'y, x, z'
'-y, x, -z'
'y, -x, -z'
'-x, -z, y'
'x, -z, -y'
'x, z, y'
'-x, z, -y'
'-z, -y, x'
'-z, y, -x'
'z, -y, -x'
'z, y, x'
'-x, -y+1/2, -z+1/2'
'x, y+1/2, -z+1/2'
'x, -y+1/2, z+1/2'
'-x, y+1/2, z+1/2'
'-z, -x+1/2, -y+1/2'
'-z, x+1/2, y+1/2'
'z, x+1/2, -y+1/2'
'z, -x+1/2, y+1/2'
'-y, -z+1/2, -x+1/2'
'y, -z+1/2, x+1/2'
'-y, z+1/2, x+1/2'
'y, z+1/2, -x+1/2'
'-y, -x+1/2, z+1/2'
'y, x+1/2, z+1/2'
'-y, x+1/2, -z+1/2'
'y, -x+1/2, -z+1/2'
'-x, -z+1/2, y+1/2'
'x, -z+1/2, -y+1/2'
'x, z+1/2, y+1/2'
'-x, z+1/2, -y+1/2'
'-z, -y+1/2, x+1/2'
'-z, y+1/2, -x+1/2'
'z, -y+1/2, -x+1/2'
'z, y+1/2, x+1/2'
'-x+1/2, -y, -z+1/2'
'x+1/2, y, -z+1/2'
'x+1/2, -y, z+1/2'
'-x+1/2, y, z+1/2'
'-z+1/2, -x, -y+1/2'
'-z+1/2, x, y+1/2'
'z+1/2, x, -y+1/2'
'z+1/2, -x, y+1/2'
'-y+1/2, -z, -x+1/2'
'y+1/2, -z, x+1/2'
'-y+1/2, z, x+1/2'
'y+1/2, z, -x+1/2'
'-y+1/2, -x, z+1/2'
'y+1/2, x, z+1/2'
'-y+1/2, x, -z+1/2'
'y+1/2, -x, -z+1/2'
'-x+1/2, -z, y+1/2'
'x+1/2, -z, -y+1/2'
'x+1/2, z, y+1/2'
'-x+1/2, z, -y+1/2'
'-z+1/2, -y, x+1/2'
'-z+1/2, y, -x+1/2'
'z+1/2, -y, -x+1/2'
'z+1/2, y, x+1/2'
'-x+1/2, -y+1/2, -z'
'x+1/2, y+1/2, -z'
'x+1/2, -y+1/2, z'
'-x+1/2, y+1/2, z'
'-z+1/2, -x+1/2, -y'
'-z+1/2, x+1/2, y'
'z+1/2, x+1/2, -y'
'z+1/2, -x+1/2, y'
'-y+1/2, -z+1/2, -x'
'y+1/2, -z+1/2, x'
'-y+1/2, z+1/2, x'
'y+1/2, z+1/2, -x'
'-y+1/2, -x+1/2, z'
'y+1/2, x+1/2, z'
'-y+1/2, x+1/2, -z'
'y+1/2, -x+1/2, -z'
'-x+1/2, -z+1/2, y'
'x+1/2, -z+1/2, -y'
'x+1/2, z+1/2, y'
'-x+1/2, z+1/2, -y'
'-z+1/2, -y+1/2, x'
'-z+1/2, y+1/2, -x'
'z+1/2, -y+1/2, -x'
'z+1/2, y+1/2, x'

_cell_length_a                   25.856(3)
_cell_length_b                   25.856(3)
_cell_length_c                   25.856(3)
_cell_angle_alpha                90.00
_cell_angle_beta                 90.00
_cell_angle_gamma                90.00
_cell_volume                     17286(3)
_cell_formula_units_Z            8
_cell_measurement_temperature    50(2)
_cell_measurement_reflns_used    ?
_cell_measurement_theta_min      ?
_cell_measurement_theta_max      ?

_exptl_crystal_description       Block
_exptl_crystal_colour            Colourless
_exptl_crystal_size_max          0.6
_exptl_crystal_size_mid          0.6
_exptl_crystal_size_min          0.4
_exptl_crystal_density_meas      'Not measured'
_exptl_crystal_density_diffrn    0.593
_exptl_crystal_density_method    'not measured'
_exptl_crystal_F_000             1583
_exptl_absorpt_coefficient_mu    0.000
_exptl_absorpt_correction_type   None
_exptl_absorpt_correction_T_min  ?
_exptl_absorpt_correction_T_max  ?
_exptl_absorpt_process_details   ?

_exptl_special_details           
;
?
;

_diffrn_ambient_temperature      50(2)
_diffrn_radiation_wavelength     0.85-3.5
_diffrn_radiation_type           Neutron
_diffrn_radiation_source         'ILL high-flux reactor'
_diffrn_radiation_monochromator  graphite
_diffrn_measurement_device_type  'VIVALDI Neutron Laue Diffractometer'
_diffrn_measurement_method       'Laue method'
_diffrn_detector_area_resol_mean ?
_diffrn_standards_number         0
_diffrn_standards_interval_count 0
_diffrn_standards_interval_time  0
_diffrn_standards_decay_%        0
_diffrn_reflns_number            4665
_diffrn_reflns_av_R_equivalents  0.3606
_diffrn_reflns_av_sigmaI/netI    0.2033
_diffrn_reflns_limit_h_min       -14
_diffrn_reflns_limit_h_max       26
_diffrn_reflns_limit_k_min       -26
_diffrn_reflns_limit_k_max       13
_diffrn_reflns_limit_l_min       -19
_diffrn_reflns_limit_l_max       19
_diffrn_reflns_theta_min         2.61
_diffrn_reflns_theta_max         21.44
_reflns_number_total             411
_reflns_number_gt                325
_reflns_threshold_expression     >2sigma(I)

_computing_data_collection       'VIVALDI Controller'
_computing_cell_refinement       'LAUEGEN (Campbell, 1998)'
_computing_data_reduction        
;
INTERGRATE & LAUENORM (Wilkinson, 1998)(Campbell, 1996)
;
_computing_structure_solution    'SHELXS-97 (Sheldrick, 1990)'
_computing_structure_refinement  'SHELXL-97 (Sheldrick, 1997)'
_computing_molecular_graphics    'OLEX (Dolomanov, 2003)'
_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.

Initially the occupancy and Uiso values for the hydrogen gas atom (H1)
were jointly refined (after separate refinement). The occupancy became
143% (approx. error of 10%) and the Uiso value was large and unrealistic.
For this reason the occupancy was fixed to 100%. This gave more
realistic Uiso values for H1.
;

_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^)+(0.0002P)^2^+0.0000P] where P=(Fo^2^+2Fc^2^)/3'
_atom_sites_solution_primary     direct
_atom_sites_solution_secondary   difmap
_atom_sites_solution_hydrogens   difmap
_refine_ls_hydrogen_treatment    refall
_refine_ls_extinction_method     none
_refine_ls_extinction_coef       'Not refined'
_refine_ls_number_reflns         411
_refine_ls_number_parameters     19
_refine_ls_number_restraints     0
_refine_ls_R_factor_all          0.2725
_refine_ls_R_factor_gt           0.2154
_refine_ls_wR_factor_ref         0.2314
_refine_ls_wR_factor_gt          0.2228
_refine_ls_goodness_of_fit_ref   1.996
_refine_ls_restrained_S_all      1.996
_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
Zn1 Zn 0.2946(3) 0.2946(3) 0.2054(3) 0.014(4) Uiso 1 6 d S . .
O1 O 0.2500 0.2500 0.2500 0.027(8) Uiso 1 24 d S . .
O2 O 0.2806(2) 0.3661(4) 0.2194(2) 0.029(3) Uiso 1 2 d S . .
C1 C 0.2500 0.3894(4) 0.2500 0.020(3) Uiso 1 4 d S . .
C2 C 0.2500 0.4449(4) 0.2500 0.012(2) Uiso 1 4 d S . .
C3 C 0.2829(2) 0.4733(3) 0.2171(2) 0.0157(18) Uiso 1 2 d S . .
H3 H 0.1931(5) 0.0475(7) 0.1931(5) 0.048(5) Uiso 1 2 d S . .
H1 H 0.3378(8) 0.1622(8) 0.1622(8) 0.092(13) Uiso 1 6 d S . .

_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
O2 C1 1.270(10) . ?
C1 O2 1.270(10) 51 ?
C1 C2 1.435(17) . ?
C2 C3 1.409(8) . ?
C2 C3 1.409(8) 51 ?
C3 C3 1.382(14) 99_565 ?

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 C1 O2 123.4(12) . 51 ?
O2 C1 C2 118.3(6) . . ?
O2 C1 C2 118.3(6) 51 . ?
C3 C2 C3 117.2(10) . 51 ?
C3 C2 C1 121.4(5) . . ?
C3 C2 C1 121.4(5) 51 . ?
C3 C3 C2 121.4(5) 99_565 . ?

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
O2 C1 C2 C3 0.000(2) . . . . ?
O2 C1 C2 C3 180.000(1) 51 . . . ?
O2 C1 C2 C3 180.000(1) . . . 51 ?
O2 C1 C2 C3 0.000(2) 51 . . 51 ?
C3 C2 C3 C3 0.000(2) 51 . . 99_565 ?
C1 C2 C3 C3 180.000(1) . . . 99_565 ?

_diffrn_measured_fraction_theta_max 0.739
_diffrn_reflns_theta_full        21.44
_diffrn_measured_fraction_theta_full 0.739
_refine_diff_density_max         0.601
_refine_diff_density_min         -0.457
_refine_diff_density_rms         0.105

data_120K
_database_code_depnum_ccdc_archive 'CCDC 282410'

_audit_creation_method           SHELXL-97
_chemical_name_systematic        
;
Hydrogen-Loaded Zn4O(1,4-Benzenedicarboxylate)
;
_chemical_name_common            
'Hydrogen-Loaded Zn4O(1,4-Benzenedicarboxylate)'
_chemical_melting_point          ?
_chemical_formula_moiety         'C24 H12 O13 Zn4'
_chemical_formula_sum            'C24 H12 O13 Zn4'
_chemical_formula_weight         768.00

loop_
_atom_type_symbol
_atom_type_description
_atom_type_scat_dispersion_real
_atom_type_scat_dispersion_imag
_atom_type_scat_source
C C 0.0000 0.0000 '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 0.0000 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'
Zn Zn 0.0000 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'

_symmetry_cell_setting           Cubic
_symmetry_space_group_name_H-M   Fm-3m
_symmetry_space_group_name_Hall  '-F 4 2 3'

loop_
_symmetry_equiv_pos_as_xyz
'x, y, z'
'-x, -y, z'
'-x, y, -z'
'x, -y, -z'
'z, x, y'
'z, -x, -y'
'-z, -x, y'
'-z, x, -y'
'y, z, x'
'-y, z, -x'
'y, -z, -x'
'-y, -z, x'
'y, x, -z'
'-y, -x, -z'
'y, -x, z'
'-y, x, z'
'x, z, -y'
'-x, z, y'
'-x, -z, -y'
'x, -z, y'
'z, y, -x'
'z, -y, x'
'-z, y, x'
'-z, -y, -x'
'x, y+1/2, z+1/2'
'-x, -y+1/2, z+1/2'
'-x, y+1/2, -z+1/2'
'x, -y+1/2, -z+1/2'
'z, x+1/2, y+1/2'
'z, -x+1/2, -y+1/2'
'-z, -x+1/2, y+1/2'
'-z, x+1/2, -y+1/2'
'y, z+1/2, x+1/2'
'-y, z+1/2, -x+1/2'
'y, -z+1/2, -x+1/2'
'-y, -z+1/2, x+1/2'
'y, x+1/2, -z+1/2'
'-y, -x+1/2, -z+1/2'
'y, -x+1/2, z+1/2'
'-y, x+1/2, z+1/2'
'x, z+1/2, -y+1/2'
'-x, z+1/2, y+1/2'
'-x, -z+1/2, -y+1/2'
'x, -z+1/2, y+1/2'
'z, y+1/2, -x+1/2'
'z, -y+1/2, x+1/2'
'-z, y+1/2, x+1/2'
'-z, -y+1/2, -x+1/2'
'x+1/2, y, z+1/2'
'-x+1/2, -y, z+1/2'
'-x+1/2, y, -z+1/2'
'x+1/2, -y, -z+1/2'
'z+1/2, x, y+1/2'
'z+1/2, -x, -y+1/2'
'-z+1/2, -x, y+1/2'
'-z+1/2, x, -y+1/2'
'y+1/2, z, x+1/2'
'-y+1/2, z, -x+1/2'
'y+1/2, -z, -x+1/2'
'-y+1/2, -z, x+1/2'
'y+1/2, x, -z+1/2'
'-y+1/2, -x, -z+1/2'
'y+1/2, -x, z+1/2'
'-y+1/2, x, z+1/2'
'x+1/2, z, -y+1/2'
'-x+1/2, z, y+1/2'
'-x+1/2, -z, -y+1/2'
'x+1/2, -z, y+1/2'
'z+1/2, y, -x+1/2'
'z+1/2, -y, x+1/2'
'-z+1/2, y, x+1/2'
'-z+1/2, -y, -x+1/2'
'x+1/2, y+1/2, z'
'-x+1/2, -y+1/2, z'
'-x+1/2, y+1/2, -z'
'x+1/2, -y+1/2, -z'
'z+1/2, x+1/2, y'
'z+1/2, -x+1/2, -y'
'-z+1/2, -x+1/2, y'
'-z+1/2, x+1/2, -y'
'y+1/2, z+1/2, x'
'-y+1/2, z+1/2, -x'
'y+1/2, -z+1/2, -x'
'-y+1/2, -z+1/2, x'
'y+1/2, x+1/2, -z'
'-y+1/2, -x+1/2, -z'
'y+1/2, -x+1/2, z'
'-y+1/2, x+1/2, z'
'x+1/2, z+1/2, -y'
'-x+1/2, z+1/2, y'
'-x+1/2, -z+1/2, -y'
'x+1/2, -z+1/2, y'
'z+1/2, y+1/2, -x'
'z+1/2, -y+1/2, x'
'-z+1/2, y+1/2, x'
'-z+1/2, -y+1/2, -x'
'-x, -y, -z'
'x, y, -z'
'x, -y, z'
'-x, y, z'
'-z, -x, -y'
'-z, x, y'
'z, x, -y'
'z, -x, y'
'-y, -z, -x'
'y, -z, x'
'-y, z, x'
'y, z, -x'
'-y, -x, z'
'y, x, z'
'-y, x, -z'
'y, -x, -z'
'-x, -z, y'
'x, -z, -y'
'x, z, y'
'-x, z, -y'
'-z, -y, x'
'-z, y, -x'
'z, -y, -x'
'z, y, x'
'-x, -y+1/2, -z+1/2'
'x, y+1/2, -z+1/2'
'x, -y+1/2, z+1/2'
'-x, y+1/2, z+1/2'
'-z, -x+1/2, -y+1/2'
'-z, x+1/2, y+1/2'
'z, x+1/2, -y+1/2'
'z, -x+1/2, y+1/2'
'-y, -z+1/2, -x+1/2'
'y, -z+1/2, x+1/2'
'-y, z+1/2, x+1/2'
'y, z+1/2, -x+1/2'
'-y, -x+1/2, z+1/2'
'y, x+1/2, z+1/2'
'-y, x+1/2, -z+1/2'
'y, -x+1/2, -z+1/2'
'-x, -z+1/2, y+1/2'
'x, -z+1/2, -y+1/2'
'x, z+1/2, y+1/2'
'-x, z+1/2, -y+1/2'
'-z, -y+1/2, x+1/2'
'-z, y+1/2, -x+1/2'
'z, -y+1/2, -x+1/2'
'z, y+1/2, x+1/2'
'-x+1/2, -y, -z+1/2'
'x+1/2, y, -z+1/2'
'x+1/2, -y, z+1/2'
'-x+1/2, y, z+1/2'
'-z+1/2, -x, -y+1/2'
'-z+1/2, x, y+1/2'
'z+1/2, x, -y+1/2'
'z+1/2, -x, y+1/2'
'-y+1/2, -z, -x+1/2'
'y+1/2, -z, x+1/2'
'-y+1/2, z, x+1/2'
'y+1/2, z, -x+1/2'
'-y+1/2, -x, z+1/2'
'y+1/2, x, z+1/2'
'-y+1/2, x, -z+1/2'
'y+1/2, -x, -z+1/2'
'-x+1/2, -z, y+1/2'
'x+1/2, -z, -y+1/2'
'x+1/2, z, y+1/2'
'-x+1/2, z, -y+1/2'
'-z+1/2, -y, x+1/2'
'-z+1/2, y, -x+1/2'
'z+1/2, -y, -x+1/2'
'z+1/2, y, x+1/2'
'-x+1/2, -y+1/2, -z'
'x+1/2, y+1/2, -z'
'x+1/2, -y+1/2, z'
'-x+1/2, y+1/2, z'
'-z+1/2, -x+1/2, -y'
'-z+1/2, x+1/2, y'
'z+1/2, x+1/2, -y'
'z+1/2, -x+1/2, y'
'-y+1/2, -z+1/2, -x'
'y+1/2, -z+1/2, x'
'-y+1/2, z+1/2, x'
'y+1/2, z+1/2, -x'
'-y+1/2, -x+1/2, z'
'y+1/2, x+1/2, z'
'-y+1/2, x+1/2, -z'
'y+1/2, -x+1/2, -z'
'-x+1/2, -z+1/2, y'
'x+1/2, -z+1/2, -y'
'x+1/2, z+1/2, y'
'-x+1/2, z+1/2, -y'
'-z+1/2, -y+1/2, x'
'-z+1/2, y+1/2, -x'
'z+1/2, -y+1/2, -x'
'z+1/2, y+1/2, x'

_cell_length_a                   25.856(3)
_cell_length_b                   25.856(3)
_cell_length_c                   25.856(3)
_cell_angle_alpha                90.00
_cell_angle_beta                 90.00
_cell_angle_gamma                90.00
_cell_volume                     17286(3)
_cell_formula_units_Z            8
_cell_measurement_temperature    120(2)
_cell_measurement_reflns_used    ?
_cell_measurement_theta_min      ?
_cell_measurement_theta_max      ?

_exptl_crystal_description       Block
_exptl_crystal_colour            Colourless
_exptl_crystal_size_max          0.6
_exptl_crystal_size_mid          0.6
_exptl_crystal_size_min          0.4
_exptl_crystal_density_meas      'Not measured'
_exptl_crystal_density_diffrn    0.590
_exptl_crystal_density_method    'not measured'
_exptl_crystal_F_000             1703
_exptl_absorpt_coefficient_mu    0.000
_exptl_absorpt_correction_type   ?
_exptl_absorpt_correction_T_min  ?
_exptl_absorpt_correction_T_max  ?
_exptl_absorpt_process_details   ?

_exptl_special_details           
;
?
;

_diffrn_ambient_temperature      120(2)
_diffrn_radiation_wavelength     0.85-3.5
_diffrn_radiation_type           Neutron
_diffrn_radiation_source         'ILL high-flux reactor'
_diffrn_radiation_monochromator  graphite
_diffrn_measurement_device_type  'VIVALDI Neutron Laue Diffractometer'
_diffrn_measurement_method       'Laue method'
_diffrn_detector_area_resol_mean ?
_diffrn_standards_number         0
_diffrn_standards_interval_count 0
_diffrn_standards_interval_time  0
_diffrn_standards_decay_%        0
_diffrn_reflns_number            5615
_diffrn_reflns_av_R_equivalents  0.4189
_diffrn_reflns_av_sigmaI/netI    0.2161
_diffrn_reflns_limit_h_min       -21
_diffrn_reflns_limit_h_max       26
_diffrn_reflns_limit_k_min       -26
_diffrn_reflns_limit_k_max       13
_diffrn_reflns_limit_l_min       -19
_diffrn_reflns_limit_l_max       18
_diffrn_reflns_theta_min         1.36
_diffrn_reflns_theta_max         21.20
_reflns_number_total             417
_reflns_number_gt                361
_reflns_threshold_expression     >2sigma(I)

_computing_data_collection       'VIVALDI Controller'
_computing_cell_refinement       'LAUEGEN (Campbell, 1998)'
_computing_data_reduction        
;
INTERGRATE & LAUENORM (Wilkinson, 1998)(Campbell, 1996)
;
_computing_structure_solution    'SHELXS-97 (Sheldrick, 1990)'
_computing_structure_refinement  'SHELXL-97 (Sheldrick, 1997)'
_computing_molecular_graphics    'OLEX (Dolomanov, 2003)'
_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^)+(0.0002P)^2^+0.0000P] where P=(Fo^2^+2Fc^2^)/3'
_atom_sites_solution_primary     direct
_atom_sites_solution_secondary   difmap
_atom_sites_solution_hydrogens   difmap
_refine_ls_hydrogen_treatment    Refall
_refine_ls_extinction_method     none
_refine_ls_extinction_coef       'Not refined'
_refine_ls_number_reflns         417
_refine_ls_number_parameters     17
_refine_ls_number_restraints     0
_refine_ls_R_factor_all          0.3042
_refine_ls_R_factor_gt           0.2721
_refine_ls_wR_factor_ref         0.2629
_refine_ls_wR_factor_gt          0.2585
_refine_ls_goodness_of_fit_ref   2.272
_refine_ls_restrained_S_all      2.272
_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
Zn1 Zn 0.2933(4) 0.2933(4) 0.2067(4) 0.021(4) Uiso 1 6 d S . .
O1 O 0.2500 0.2500 0.2500 0.026(9) Uiso 1 24 d S . .
O2 O 0.2805(3) 0.3657(4) 0.2195(3) 0.037(3) Uiso 1 2 d S . .
C1 C 0.2500 0.3893(5) 0.2500 0.024(3) Uiso 1 4 d S . .
C2 C 0.2500 0.4458(5) 0.2500 0.028(3) Uiso 1 4 d S . .
C3 C 0.2826(3) 0.4730(3) 0.2174(3) 0.031(2) Uiso 1 2 d S . .
H3 H 0.1934(7) 0.0494(9) 0.1934(7) 0.067(6) Uiso 1 2 d S . .

_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
O2 C1 1.272(12) . ?
C1 O2 1.272(12) 51 ?
C1 C2 1.46(2) . ?
C2 C3 1.383(11) 51 ?
C2 C3 1.383(11) . ?
C3 C3 1.399(17) 99_565 ?

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 C1 O2 122.7(14) 51 . ?
O2 C1 C2 118.7(7) 51 . ?
O2 C1 C2 118.7(7) . . ?
C3 C2 C3 119.1(13) 51 . ?
C3 C2 C1 120.5(6) 51 . ?
C3 C2 C1 120.5(6) . . ?
C2 C3 C3 120.5(6) . 99_565 ?

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
O2 C1 C2 C3 0.000(2) 51 . . 51 ?
O2 C1 C2 C3 180.000(2) . . . 51 ?
O2 C1 C2 C3 180.000(2) 51 . . . ?
O2 C1 C2 C3 0.000(2) . . . . ?
C3 C2 C3 C3 0.000(3) 51 . . 99_565 ?
C1 C2 C3 C3 180.000(2) . . . 99_565 ?

_diffrn_measured_fraction_theta_max 0.768
_diffrn_reflns_theta_full        21.20
_diffrn_measured_fraction_theta_full 0.768
_refine_diff_density_max         0.565
_refine_diff_density_min         -0.464
_refine_diff_density_rms         0.103

data_150K
_database_code_depnum_ccdc_archive 'CCDC 282411'

_audit_creation_method           SHELXL-97
_chemical_name_systematic        
;
Hydrogen-Loaded Zn4O(1,4-Benzenedicarboxylate)
;
_chemical_name_common            
'Hydrogen-Loaded Zn4O(1,4-Benzenedicarboxylate)'
_chemical_melting_point          ?
_chemical_formula_moiety         'C24 H12 O13 Zn4'
_chemical_formula_sum            'C24 H12 O13 Zn4'
_chemical_formula_weight         768.00

loop_
_atom_type_symbol
_atom_type_description
_atom_type_scat_dispersion_real
_atom_type_scat_dispersion_imag
_atom_type_scat_source
C C 0.0000 0.0000 '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 0.0000 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'
Zn Zn 0.0000 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'

_symmetry_cell_setting           Cubic
_symmetry_space_group_name_H-M   Fm-3m
_symmetry_space_group_name_Hall  '-F 4 2 3'

loop_
_symmetry_equiv_pos_as_xyz
'x, y, z'
'-x, -y, z'
'-x, y, -z'
'x, -y, -z'
'z, x, y'
'z, -x, -y'
'-z, -x, y'
'-z, x, -y'
'y, z, x'
'-y, z, -x'
'y, -z, -x'
'-y, -z, x'
'y, x, -z'
'-y, -x, -z'
'y, -x, z'
'-y, x, z'
'x, z, -y'
'-x, z, y'
'-x, -z, -y'
'x, -z, y'
'z, y, -x'
'z, -y, x'
'-z, y, x'
'-z, -y, -x'
'x, y+1/2, z+1/2'
'-x, -y+1/2, z+1/2'
'-x, y+1/2, -z+1/2'
'x, -y+1/2, -z+1/2'
'z, x+1/2, y+1/2'
'z, -x+1/2, -y+1/2'
'-z, -x+1/2, y+1/2'
'-z, x+1/2, -y+1/2'
'y, z+1/2, x+1/2'
'-y, z+1/2, -x+1/2'
'y, -z+1/2, -x+1/2'
'-y, -z+1/2, x+1/2'
'y, x+1/2, -z+1/2'
'-y, -x+1/2, -z+1/2'
'y, -x+1/2, z+1/2'
'-y, x+1/2, z+1/2'
'x, z+1/2, -y+1/2'
'-x, z+1/2, y+1/2'
'-x, -z+1/2, -y+1/2'
'x, -z+1/2, y+1/2'
'z, y+1/2, -x+1/2'
'z, -y+1/2, x+1/2'
'-z, y+1/2, x+1/2'
'-z, -y+1/2, -x+1/2'
'x+1/2, y, z+1/2'
'-x+1/2, -y, z+1/2'
'-x+1/2, y, -z+1/2'
'x+1/2, -y, -z+1/2'
'z+1/2, x, y+1/2'
'z+1/2, -x, -y+1/2'
'-z+1/2, -x, y+1/2'
'-z+1/2, x, -y+1/2'
'y+1/2, z, x+1/2'
'-y+1/2, z, -x+1/2'
'y+1/2, -z, -x+1/2'
'-y+1/2, -z, x+1/2'
'y+1/2, x, -z+1/2'
'-y+1/2, -x, -z+1/2'
'y+1/2, -x, z+1/2'
'-y+1/2, x, z+1/2'
'x+1/2, z, -y+1/2'
'-x+1/2, z, y+1/2'
'-x+1/2, -z, -y+1/2'
'x+1/2, -z, y+1/2'
'z+1/2, y, -x+1/2'
'z+1/2, -y, x+1/2'
'-z+1/2, y, x+1/2'
'-z+1/2, -y, -x+1/2'
'x+1/2, y+1/2, z'
'-x+1/2, -y+1/2, z'
'-x+1/2, y+1/2, -z'
'x+1/2, -y+1/2, -z'
'z+1/2, x+1/2, y'
'z+1/2, -x+1/2, -y'
'-z+1/2, -x+1/2, y'
'-z+1/2, x+1/2, -y'
'y+1/2, z+1/2, x'
'-y+1/2, z+1/2, -x'
'y+1/2, -z+1/2, -x'
'-y+1/2, -z+1/2, x'
'y+1/2, x+1/2, -z'
'-y+1/2, -x+1/2, -z'
'y+1/2, -x+1/2, z'
'-y+1/2, x+1/2, z'
'x+1/2, z+1/2, -y'
'-x+1/2, z+1/2, y'
'-x+1/2, -z+1/2, -y'
'x+1/2, -z+1/2, y'
'z+1/2, y+1/2, -x'
'z+1/2, -y+1/2, x'
'-z+1/2, y+1/2, x'
'-z+1/2, -y+1/2, -x'
'-x, -y, -z'
'x, y, -z'
'x, -y, z'
'-x, y, z'
'-z, -x, -y'
'-z, x, y'
'z, x, -y'
'z, -x, y'
'-y, -z, -x'
'y, -z, x'
'-y, z, x'
'y, z, -x'
'-y, -x, z'
'y, x, z'
'-y, x, -z'
'y, -x, -z'
'-x, -z, y'
'x, -z, -y'
'x, z, y'
'-x, z, -y'
'-z, -y, x'
'-z, y, -x'
'z, -y, -x'
'z, y, x'
'-x, -y+1/2, -z+1/2'
'x, y+1/2, -z+1/2'
'x, -y+1/2, z+1/2'
'-x, y+1/2, z+1/2'
'-z, -x+1/2, -y+1/2'
'-z, x+1/2, y+1/2'
'z, x+1/2, -y+1/2'
'z, -x+1/2, y+1/2'
'-y, -z+1/2, -x+1/2'
'y, -z+1/2, x+1/2'
'-y, z+1/2, x+1/2'
'y, z+1/2, -x+1/2'
'-y, -x+1/2, z+1/2'
'y, x+1/2, z+1/2'
'-y, x+1/2, -z+1/2'
'y, -x+1/2, -z+1/2'
'-x, -z+1/2, y+1/2'
'x, -z+1/2, -y+1/2'
'x, z+1/2, y+1/2'
'-x, z+1/2, -y+1/2'
'-z, -y+1/2, x+1/2'
'-z, y+1/2, -x+1/2'
'z, -y+1/2, -x+1/2'
'z, y+1/2, x+1/2'
'-x+1/2, -y, -z+1/2'
'x+1/2, y, -z+1/2'
'x+1/2, -y, z+1/2'
'-x+1/2, y, z+1/2'
'-z+1/2, -x, -y+1/2'
'-z+1/2, x, y+1/2'
'z+1/2, x, -y+1/2'
'z+1/2, -x, y+1/2'
'-y+1/2, -z, -x+1/2'
'y+1/2, -z, x+1/2'
'-y+1/2, z, x+1/2'
'y+1/2, z, -x+1/2'
'-y+1/2, -x, z+1/2'
'y+1/2, x, z+1/2'
'-y+1/2, x, -z+1/2'
'y+1/2, -x, -z+1/2'
'-x+1/2, -z, y+1/2'
'x+1/2, -z, -y+1/2'
'x+1/2, z, y+1/2'
'-x+1/2, z, -y+1/2'
'-z+1/2, -y, x+1/2'
'-z+1/2, y, -x+1/2'
'z+1/2, -y, -x+1/2'
'z+1/2, y, x+1/2'
'-x+1/2, -y+1/2, -z'
'x+1/2, y+1/2, -z'
'x+1/2, -y+1/2, z'
'-x+1/2, y+1/2, z'
'-z+1/2, -x+1/2, -y'
'-z+1/2, x+1/2, y'
'z+1/2, x+1/2, -y'
'z+1/2, -x+1/2, y'
'-y+1/2, -z+1/2, -x'
'y+1/2, -z+1/2, x'
'-y+1/2, z+1/2, x'
'y+1/2, z+1/2, -x'
'-y+1/2, -x+1/2, z'
'y+1/2, x+1/2, z'
'-y+1/2, x+1/2, -z'
'y+1/2, -x+1/2, -z'
'-x+1/2, -z+1/2, y'
'x+1/2, -z+1/2, -y'
'x+1/2, z+1/2, y'
'-x+1/2, z+1/2, -y'
'-z+1/2, -y+1/2, x'
'-z+1/2, y+1/2, -x'
'z+1/2, -y+1/2, -x'
'z+1/2, y+1/2, x'

_cell_length_a                   25.8878(4)
_cell_length_b                   25.8878(4)
_cell_length_c                   25.8878(4)
_cell_angle_alpha                90.00
_cell_angle_beta                 90.00
_cell_angle_gamma                90.00
_cell_volume                     17349.4(5)
_cell_formula_units_Z            8
_cell_measurement_temperature    150(2)
_cell_measurement_reflns_used    ?
_cell_measurement_theta_min      ?
_cell_measurement_theta_max      ?

_exptl_crystal_description       Block
_exptl_crystal_colour            Colourless
_exptl_crystal_size_max          0.6
_exptl_crystal_size_mid          0.6
_exptl_crystal_size_min          0.4
_exptl_crystal_density_meas      'Not measured'
_exptl_crystal_density_diffrn    0.588
_exptl_crystal_density_method    'not measured'
_exptl_crystal_F_000             1703
_exptl_absorpt_coefficient_mu    0.000
_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     0.85-3.5
_diffrn_radiation_type           Neutron
_diffrn_radiation_source         'ILL high-flux reactor'
_diffrn_radiation_monochromator  graphite
_diffrn_measurement_device_type  'VIVALDI Neutron Laue Diffractometer'
_diffrn_measurement_method       'Laue method'
_diffrn_detector_area_resol_mean ?
_diffrn_standards_number         0
_diffrn_standards_interval_count 0
_diffrn_standards_interval_time  0
_diffrn_standards_decay_%        0
_diffrn_reflns_number            3712
_diffrn_reflns_av_R_equivalents  0.4422
_diffrn_reflns_av_sigmaI/netI    0.3135
_diffrn_reflns_limit_h_min       -14
_diffrn_reflns_limit_h_max       26
_diffrn_reflns_limit_k_min       -26
_diffrn_reflns_limit_k_max       12
_diffrn_reflns_limit_l_min       -18
_diffrn_reflns_limit_l_max       18
_diffrn_reflns_theta_min         1.36
_diffrn_reflns_theta_max         21.17
_reflns_number_total             403
_reflns_number_gt                288
_reflns_threshold_expression     >2sigma(I)

_computing_data_collection       'VIVALDI Controller'
_computing_cell_refinement       'LAUEGEN (Campbell, 1998)'
_computing_data_reduction        
;
INTERGRATE & LAUENORM (Wilkinson, 1998)(Campbell, 1996)
;
_computing_structure_solution    'SHELXS-97 (Sheldrick, 1990)'
_computing_structure_refinement  'SHELXL-97 (Sheldrick, 1997)'
_computing_molecular_graphics    'OLEX (Dolomanov, 2003)'
_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^)+(0.0001P)^2^+0.0000P] where P=(Fo^2^+2Fc^2^)/3'
_atom_sites_solution_primary     direct
_atom_sites_solution_secondary   difmap
_atom_sites_solution_hydrogens   difmap
_refine_ls_hydrogen_treatment    refall
_refine_ls_extinction_method     none
_refine_ls_extinction_coef       'Not refined'
_refine_ls_number_reflns         403
_refine_ls_number_parameters     17
_refine_ls_number_restraints     0
_refine_ls_R_factor_all          0.3704
_refine_ls_R_factor_gt           0.3039
_refine_ls_wR_factor_ref         0.3093
_refine_ls_wR_factor_gt          0.2941
_refine_ls_goodness_of_fit_ref   1.921
_refine_ls_restrained_S_all      1.921
_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
Zn1 Zn 0.2938(5) 0.2938(5) 0.2062(5) 0.024(6) Uiso 1 6 d S . .
O1 O 0.2500 0.2500 0.2500 0.050(16) Uiso 1 24 d S . .
O2 O 0.2806(4) 0.3661(6) 0.2194(4) 0.050(5) Uiso 1 2 d S . .
C1 C 0.2500 0.3915(7) 0.2500 0.029(4) Uiso 1 4 d S . .
C2 C 0.2500 0.4450(7) 0.2500 0.044(5) Uiso 1 4 d S . .
C3 C 0.2829(3) 0.4739(4) 0.2171(3) 0.031(3) Uiso 1 2 d S . .
H3 H 0.1940(10) 0.0491(14) 0.1940(10) 0.095(11) Uiso 1 2 d S . .

_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
O2 C1 1.299(17) . ?
C1 O2 1.299(17) 51 ?
C1 C2 1.38(3) . ?
C2 C3 1.417(15) 51 ?
C2 C3 1.417(15) . ?
C3 C3 1.35(2) 99_565 ?

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 C1 O2 119(2) 51 . ?
O2 C1 C2 120.5(10) 51 . ?
O2 C1 C2 120.5(10) . . ?
C1 C2 C3 121.9(9) . 51 ?
C1 C2 C3 121.9(9) . . ?
C3 C2 C3 116.3(17) 51 . ?
C3 C3 C2 121.9(9) 99_565 . ?

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
O2 C1 C2 C3 0.000(3) 51 . . 51 ?
O2 C1 C2 C3 180.000(2) . . . 51 ?
O2 C1 C2 C3 180.000(2) 51 . . . ?
O2 C1 C2 C3 0.000(3) . . . . ?
C1 C2 C3 C3 180.000(2) . . . 99_565 ?
C3 C2 C3 C3 0.000(3) 51 . . 99_565 ?

_diffrn_measured_fraction_theta_max 0.742
_diffrn_reflns_theta_full        21.17
_diffrn_measured_fraction_theta_full 0.742
_refine_diff_density_max         0.583
_refine_diff_density_min         -0.548
_refine_diff_density_rms         0.105

data_300K
_database_code_depnum_ccdc_archive 'CCDC 282412'

_audit_creation_method           SHELXL-97
_chemical_name_systematic        
;
Hydrogen-Loaded Zn4O(1,4-Benzenedicarboxylate)
;
_chemical_name_common            
'Hydrogen-Loaded Zn4O(1,4-Benzenedicarboxylate)'
_chemical_melting_point          ?
_chemical_formula_moiety         'C24 H12 O13 Zn4'
_chemical_formula_sum            'C24 H12 O13 Zn4'
_chemical_formula_weight         768.00

loop_
_atom_type_symbol
_atom_type_description
_atom_type_scat_dispersion_real
_atom_type_scat_dispersion_imag
_atom_type_scat_source
C C 0.0000 0.0000 '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 0.0000 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'
Zn Zn 0.0000 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'

_symmetry_cell_setting           Cubic
_symmetry_space_group_name_H-M   Fm-3m
_symmetry_space_group_name_Hall  '-F 4 2 3'

loop_
_symmetry_equiv_pos_as_xyz
'x, y, z'
'-x, -y, z'
'-x, y, -z'
'x, -y, -z'
'z, x, y'
'z, -x, -y'
'-z, -x, y'
'-z, x, -y'
'y, z, x'
'-y, z, -x'
'y, -z, -x'
'-y, -z, x'
'y, x, -z'
'-y, -x, -z'
'y, -x, z'
'-y, x, z'
'x, z, -y'
'-x, z, y'
'-x, -z, -y'
'x, -z, y'
'z, y, -x'
'z, -y, x'
'-z, y, x'
'-z, -y, -x'
'x, y+1/2, z+1/2'
'-x, -y+1/2, z+1/2'
'-x, y+1/2, -z+1/2'
'x, -y+1/2, -z+1/2'
'z, x+1/2, y+1/2'
'z, -x+1/2, -y+1/2'
'-z, -x+1/2, y+1/2'
'-z, x+1/2, -y+1/2'
'y, z+1/2, x+1/2'
'-y, z+1/2, -x+1/2'
'y, -z+1/2, -x+1/2'
'-y, -z+1/2, x+1/2'
'y, x+1/2, -z+1/2'
'-y, -x+1/2, -z+1/2'
'y, -x+1/2, z+1/2'
'-y, x+1/2, z+1/2'
'x, z+1/2, -y+1/2'
'-x, z+1/2, y+1/2'
'-x, -z+1/2, -y+1/2'
'x, -z+1/2, y+1/2'
'z, y+1/2, -x+1/2'
'z, -y+1/2, x+1/2'
'-z, y+1/2, x+1/2'
'-z, -y+1/2, -x+1/2'
'x+1/2, y, z+1/2'
'-x+1/2, -y, z+1/2'
'-x+1/2, y, -z+1/2'
'x+1/2, -y, -z+1/2'
'z+1/2, x, y+1/2'
'z+1/2, -x, -y+1/2'
'-z+1/2, -x, y+1/2'
'-z+1/2, x, -y+1/2'
'y+1/2, z, x+1/2'
'-y+1/2, z, -x+1/2'
'y+1/2, -z, -x+1/2'
'-y+1/2, -z, x+1/2'
'y+1/2, x, -z+1/2'
'-y+1/2, -x, -z+1/2'
'y+1/2, -x, z+1/2'
'-y+1/2, x, z+1/2'
'x+1/2, z, -y+1/2'
'-x+1/2, z, y+1/2'
'-x+1/2, -z, -y+1/2'
'x+1/2, -z, y+1/2'
'z+1/2, y, -x+1/2'
'z+1/2, -y, x+1/2'
'-z+1/2, y, x+1/2'
'-z+1/2, -y, -x+1/2'
'x+1/2, y+1/2, z'
'-x+1/2, -y+1/2, z'
'-x+1/2, y+1/2, -z'
'x+1/2, -y+1/2, -z'
'z+1/2, x+1/2, y'
'z+1/2, -x+1/2, -y'
'-z+1/2, -x+1/2, y'
'-z+1/2, x+1/2, -y'
'y+1/2, z+1/2, x'
'-y+1/2, z+1/2, -x'
'y+1/2, -z+1/2, -x'
'-y+1/2, -z+1/2, x'
'y+1/2, x+1/2, -z'
'-y+1/2, -x+1/2, -z'
'y+1/2, -x+1/2, z'
'-y+1/2, x+1/2, z'
'x+1/2, z+1/2, -y'
'-x+1/2, z+1/2, y'
'-x+1/2, -z+1/2, -y'
'x+1/2, -z+1/2, y'
'z+1/2, y+1/2, -x'
'z+1/2, -y+1/2, x'
'-z+1/2, y+1/2, x'
'-z+1/2, -y+1/2, -x'
'-x, -y, -z'
'x, y, -z'
'x, -y, z'
'-x, y, z'
'-z, -x, -y'
'-z, x, y'
'z, x, -y'
'z, -x, y'
'-y, -z, -x'
'y, -z, x'
'-y, z, x'
'y, z, -x'
'-y, -x, z'
'y, x, z'
'-y, x, -z'
'y, -x, -z'
'-x, -z, y'
'x, -z, -y'
'x, z, y'
'-x, z, -y'
'-z, -y, x'
'-z, y, -x'
'z, -y, -x'
'z, y, x'
'-x, -y+1/2, -z+1/2'
'x, y+1/2, -z+1/2'
'x, -y+1/2, z+1/2'
'-x, y+1/2, z+1/2'
'-z, -x+1/2, -y+1/2'
'-z, x+1/2, y+1/2'
'z, x+1/2, -y+1/2'
'z, -x+1/2, y+1/2'
'-y, -z+1/2, -x+1/2'
'y, -z+1/2, x+1/2'
'-y, z+1/2, x+1/2'
'y, z+1/2, -x+1/2'
'-y, -x+1/2, z+1/2'
'y, x+1/2, z+1/2'
'-y, x+1/2, -z+1/2'
'y, -x+1/2, -z+1/2'
'-x, -z+1/2, y+1/2'
'x, -z+1/2, -y+1/2'
'x, z+1/2, y+1/2'
'-x, z+1/2, -y+1/2'
'-z, -y+1/2, x+1/2'
'-z, y+1/2, -x+1/2'
'z, -y+1/2, -x+1/2'
'z, y+1/2, x+1/2'
'-x+1/2, -y, -z+1/2'
'x+1/2, y, -z+1/2'
'x+1/2, -y, z+1/2'
'-x+1/2, y, z+1/2'
'-z+1/2, -x, -y+1/2'
'-z+1/2, x, y+1/2'
'z+1/2, x, -y+1/2'
'z+1/2, -x, y+1/2'
'-y+1/2, -z, -x+1/2'
'y+1/2, -z, x+1/2'
'-y+1/2, z, x+1/2'
'y+1/2, z, -x+1/2'
'-y+1/2, -x, z+1/2'
'y+1/2, x, z+1/2'
'-y+1/2, x, -z+1/2'
'y+1/2, -x, -z+1/2'
'-x+1/2, -z, y+1/2'
'x+1/2, -z, -y+1/2'
'x+1/2, z, y+1/2'
'-x+1/2, z, -y+1/2'
'-z+1/2, -y, x+1/2'
'-z+1/2, y, -x+1/2'
'z+1/2, -y, -x+1/2'
'z+1/2, y, x+1/2'
'-x+1/2, -y+1/2, -z'
'x+1/2, y+1/2, -z'
'x+1/2, -y+1/2, z'
'-x+1/2, y+1/2, z'
'-z+1/2, -x+1/2, -y'
'-z+1/2, x+1/2, y'
'z+1/2, x+1/2, -y'
'z+1/2, -x+1/2, y'
'-y+1/2, -z+1/2, -x'
'y+1/2, -z+1/2, x'
'-y+1/2, z+1/2, x'
'y+1/2, z+1/2, -x'
'-y+1/2, -x+1/2, z'
'y+1/2, x+1/2, z'
'-y+1/2, x+1/2, -z'
'y+1/2, -x+1/2, -z'
'-x+1/2, -z+1/2, y'
'x+1/2, -z+1/2, -y'
'x+1/2, z+1/2, y'
'-x+1/2, z+1/2, -y'
'-z+1/2, -y+1/2, x'
'-z+1/2, y+1/2, -x'
'z+1/2, -y+1/2, -x'
'z+1/2, y+1/2, x'

_cell_length_a                   25.8878(4)
_cell_length_b                   25.8878(4)
_cell_length_c                   25.8878(4)
_cell_angle_alpha                90.00
_cell_angle_beta                 90.00
_cell_angle_gamma                90.00
_cell_volume                     17349.4(5)
_cell_formula_units_Z            8
_cell_measurement_temperature    300(2)
_cell_measurement_reflns_used    ?
_cell_measurement_theta_min      ?
_cell_measurement_theta_max      ?

_exptl_crystal_description       Block
_exptl_crystal_colour            Colourless
_exptl_crystal_size_max          0.6
_exptl_crystal_size_mid          0.6
_exptl_crystal_size_min          0.4
_exptl_crystal_density_meas      'Not measured'
_exptl_crystal_density_diffrn    0.588
_exptl_crystal_density_method    'not measured'
_exptl_crystal_F_000             1703
_exptl_absorpt_coefficient_mu    0.000
_exptl_absorpt_correction_type   None
_exptl_absorpt_correction_T_min  ?
_exptl_absorpt_correction_T_max  ?
_exptl_absorpt_process_details   ?

_exptl_special_details           
;
?
;

_diffrn_ambient_temperature      300(2)
_diffrn_radiation_wavelength     0.85-3.5
_diffrn_radiation_type           Neutron
_diffrn_radiation_source         'ILL high-flux reactor'
_diffrn_radiation_monochromator  graphite
_diffrn_measurement_device_type  'VIVALDI Neutron Laue Diffractometer'
_diffrn_measurement_method       'Laue method'
_diffrn_detector_area_resol_mean ?
_diffrn_standards_number         0
_diffrn_standards_interval_count 0
_diffrn_standards_interval_time  0
_diffrn_standards_decay_%        0
_diffrn_reflns_number            4594
_diffrn_reflns_av_R_equivalents  0.4590
_diffrn_reflns_av_sigmaI/netI    0.2770
_diffrn_reflns_limit_h_min       -20
_diffrn_reflns_limit_h_max       26
_diffrn_reflns_limit_k_min       -26
_diffrn_reflns_limit_k_max       13
_diffrn_reflns_limit_l_min       -19
_diffrn_reflns_limit_l_max       18
_diffrn_reflns_theta_min         2.23
_diffrn_reflns_theta_max         21.17
_reflns_number_total             404
_reflns_number_gt                334
_reflns_threshold_expression     >2sigma(I)

_computing_data_collection       'VIVALDI Controller'
_computing_cell_refinement       'LAUEGEN (Campbell, 1998)'
_computing_data_reduction        
;
INTERGRATE & LAUENORM (Wilkinson, 1998)(Campbell, 1996)
;
_computing_structure_solution    'SHELXS-97 (Sheldrick, 1990)'
_computing_structure_refinement  'SHELXL-97 (Sheldrick, 1997)'
_computing_molecular_graphics    'OLEX (Dolomanov, 2003)'
_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^)+(0.0001P)^2^+0.0000P] where P=(Fo^2^+2Fc^2^)/3'
_atom_sites_solution_primary     direct
_atom_sites_solution_secondary   difmap
_atom_sites_solution_hydrogens   difmap
_refine_ls_hydrogen_treatment    refall
_refine_ls_extinction_method     none
_refine_ls_extinction_coef       'Not refined'
_refine_ls_number_reflns         404
_refine_ls_number_parameters     21
_refine_ls_number_restraints     0
_refine_ls_R_factor_all          0.3905
_refine_ls_R_factor_gt           0.3583
_refine_ls_wR_factor_ref         0.2768
_refine_ls_wR_factor_gt          0.2703
_refine_ls_goodness_of_fit_ref   2.247
_refine_ls_restrained_S_all      2.247
_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
Zn1 Zn 0.2943(4) 0.2943(4) 0.2057(4) 0.026(5) Uani 1 6 d S . .
O1 O 0.2500 0.2500 0.2500 0.069(17) Uani 1 24 d S . .
O2 O 0.2814(3) 0.3664(5) 0.2186(3) 0.080(6) Uani 1 2 d S . .
C1 C 0.2500 0.3854(7) 0.2500 0.048(5) Uiso 1 4 d S . .
C2 C 0.2500 0.4459(8) 0.2500 0.070(6) Uiso 1 4 d S . .
C3 C 0.2837(4) 0.4718(5) 0.2163(4) 0.059(4) Uiso 1 2 d S . .
H3 H 0.1975(8) 0.0430(11) 0.1975(8) 0.085(10) 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
Zn1 0.026(5) 0.026(5) 0.026(5) -0.008(6) -0.008(6) 0.008(6)
O1 0.069(17) 0.069(17) 0.069(17) 0.000 0.000 0.000
O2 0.086(9) 0.069(12) 0.086(9) 0.006(6) 0.057(12) -0.006(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
O2 C1 1.251(14) . ?
C1 O2 1.251(14) 51 ?
C1 C2 1.57(3) . ?
C2 C3 1.405(16) 51 ?
C2 C3 1.405(16) . ?
C3 C3 1.46(2) 99_565 ?

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 C1 O2 134(2) 51 . ?
O2 C1 C2 113.1(11) 51 . ?
O2 C1 C2 113.1(11) . . ?
C3 C2 C3 123(2) 51 . ?
C3 C2 C1 118.5(10) 51 . ?
C3 C2 C1 118.5(10) . . ?
C2 C3 C3 118.5(10) . 99_565 ?

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
O2 C1 C2 C3 0.000(3) 51 . . 51 ?
O2 C1 C2 C3 180.000(2) . . . 51 ?
O2 C1 C2 C3 180.000(2) 51 . . . ?
O2 C1 C2 C3 0.000(3) . . . . ?
C3 C2 C3 C3 0.000(4) 51 . . 99_565 ?
C1 C2 C3 C3 180.000(2) . . . 99_565 ?

_diffrn_measured_fraction_theta_max 0.744
_diffrn_reflns_theta_full        21.17
_diffrn_measured_fraction_theta_full 0.744
_refine_diff_density_max         0.452
_refine_diff_density_min         -0.383
_refine_diff_density_rms         0.080