#------------------------------------------------------------------------------
#$Date: 2022-02-23 12:09:43 +0200 (Wed, 23 Feb 2022) $
#$Revision: 273129 $
#$URL: file:///home/coder/svn-repositories/cod/cif/4/51/35/4513572.cif $
#------------------------------------------------------------------------------
#
# This file is available in the Crystallography Open Database (COD),
# http://www.crystallography.net/
#
# All data on this site have been placed in the public domain by the
# contributors.
#
data_4513572
loop_
_publ_author_name
'Guńka, Piotr A.'
'Dziubek, Kamil F.'
'Gładysiak, Andrzej'
'Dranka, Maciej'
'Piechota, Jacek'
'Hanfland, Michael'
'Katrusiak, Andrzej'
'Zachara, Janusz'
_publ_section_title
;
 Compressed Arsenolite As4O6and Its Helium Clathrate As4O6·2He
;
_journal_issue                   8
_journal_name_full               'Crystal Growth & Design'
_journal_page_first              3740
_journal_paper_doi               10.1021/acs.cgd.5b00390
_journal_volume                  15
_journal_year                    2015
_chemical_formula_moiety         'As4 O6'
_chemical_formula_sum            'As4 O6'
_chemical_formula_weight         395.69
_chemical_name_common            arsenolite
_space_group_crystal_system      cubic
_space_group_IT_number           227
_space_group_name_Hall           '-F 4vw 2vw 3'
_space_group_name_H-M_alt        'F d -3 m :2'
_symmetry_space_group_name_Hall  '-F 4vw 2vw 3'
_symmetry_space_group_name_H-M   'F d -3 m :2'
_atom_sites_solution_primary     direct
_audit_creation_date             2014-10-15
_audit_creation_method
;
Olex2 1.2-beta
(compiled 2014.09.19 svn.r3010 for OlexSys, GUI svn.r4874)
;
_cell_angle_alpha                90
_cell_angle_beta                 90
_cell_angle_gamma                90
_cell_formula_units_Z            8
_cell_length_a                   10.3877(3)
_cell_length_b                   10.3877(3)
_cell_length_c                   10.3877(3)
_cell_measurement_pressure       4.64e6(9)
_cell_measurement_reflns_used    441
_cell_measurement_temperature    293(2)
_cell_measurement_theta_max      20.1800
_cell_measurement_theta_min      1.9710
_cell_volume                     1120.88(6)
_computing_cell_refinement
;
CrysAlisPro, Agilent Technologies,
Version 1.171.37.34 (release 22-05-2014 CrysAlis171 .NET)
(compiled May 22 2014,16:03:01)
;
_computing_data_collection
;
CrysAlisPro, Agilent Technologies,
Version 1.171.37.34 (release 22-05-2014 CrysAlis171 .NET)
(compiled May 22 2014,16:03:01)
;
_computing_data_reduction
;
CrysAlisPro, Agilent Technologies,
Version 1.171.37.34 (release 22-05-2014 CrysAlis171 .NET)
(compiled May 22 2014,16:03:01)
;
_computing_molecular_graphics    'Olex2 (Dolomanov et al., 2009)'
_computing_publication_material  'Olex2 (Dolomanov et al., 2009)'
_computing_structure_refinement  'ShelXL (Sheldrick, 2008)'
_computing_structure_solution    'ShelXT (Sheldrick, 2008)'
_diffrn_ambient_environment      He
_diffrn_ambient_pressure         4.64e6(9)
_diffrn_ambient_temperature      293(2)
_diffrn_detector                 'CCD plate'
_diffrn_measured_fraction_theta_full 0.913
_diffrn_measured_fraction_theta_max 0.704
_diffrn_measurement_details
;
  1 phi    148.00  212.00   0.5000    1.0000
omega____ theta____ kappa____ phi______ frames
   0.0000    0.0000    0.0000     -     128
;
_diffrn_measurement_device       'abstract diffractometer'
_diffrn_measurement_device_type
'MAR-CrysAlisPro-abstract goniometer: imported MAR images'
_diffrn_measurement_method       'π scans'
_diffrn_orient_matrix_UB_11      -0.0323967000
_diffrn_orient_matrix_UB_12      -0.0233210000
_diffrn_orient_matrix_UB_13      -0.0005703000
_diffrn_orient_matrix_UB_21      -0.0153440000
_diffrn_orient_matrix_UB_22      0.0220311000
_diffrn_orient_matrix_UB_23      -0.0294411000
_diffrn_orient_matrix_UB_31      0.0175103000
_diffrn_orient_matrix_UB_32      -0.0236767000
_diffrn_orient_matrix_UB_33      -0.0268877000
_diffrn_radiation_monochromator  synchrotron
_diffrn_radiation_probe          x-ray
_diffrn_radiation_wavelength     0.41427
_diffrn_reflns_av_R_equivalents  0.0330
_diffrn_reflns_av_unetI/netI     0.0226
_diffrn_reflns_laue_measured_fraction_full 0.913
_diffrn_reflns_laue_measured_fraction_max 0.704
_diffrn_reflns_limit_h_max       11
_diffrn_reflns_limit_h_min       -10
_diffrn_reflns_limit_k_max       15
_diffrn_reflns_limit_k_min       -14
_diffrn_reflns_limit_l_max       17
_diffrn_reflns_limit_l_min       -17
_diffrn_reflns_number            553
_diffrn_reflns_point_group_measured_fraction_full 0.913
_diffrn_reflns_point_group_measured_fraction_max 0.704
_diffrn_reflns_theta_full        14.392
_diffrn_reflns_theta_max         20.170
_diffrn_reflns_theta_min         1.979
_diffrn_source                   synchrotron
_exptl_absorpt_coefficient_mu    5.418
_exptl_absorpt_correction_T_max  1.00000
_exptl_absorpt_correction_T_min  0.39916
_exptl_absorpt_correction_type   multi-scan
_exptl_absorpt_process_details
;
CrysAlisPro, Agilent Technologies,
Version 1.171.37.34 (release 22-05-2014 CrysAlis171 .NET)
(compiled May 22 2014,16:03:01)
Empirical absorption correction using spherical harmonics,
 implemented in SCALE3 ABSPACK scaling algorithm.
;
_exptl_crystal_density_diffrn    4.690
_exptl_crystal_description       block
_exptl_crystal_F_000             1440
_exptl_crystal_size_max          0.065
_exptl_crystal_size_mid          0.04
_exptl_crystal_size_min          0.02
_refine_diff_density_max         1.077
_refine_diff_density_min         -1.071
_refine_diff_density_rms         0.232
_refine_ls_extinction_method     none
_refine_ls_goodness_of_fit_ref   1.294
_refine_ls_hydrogen_treatment    undef
_refine_ls_matrix_type           full
_refine_ls_number_parameters     8
_refine_ls_number_reflns         114
_refine_ls_number_restraints     0
_refine_ls_restrained_S_all      1.294
_refine_ls_R_factor_all          0.0346
_refine_ls_R_factor_gt           0.0333
_refine_ls_shift/su_max          0.000
_refine_ls_shift/su_mean         0.000
_refine_ls_structure_factor_coef Fsqd
_refine_ls_weighting_details
'w=1/[σ²(Fo²)+(0.0466P)²+21.2185P] where P=(Fo²+2Fc²)/3'
_refine_ls_weighting_scheme      calc
_refine_ls_wR_factor_gt          0.0886
_refine_ls_wR_factor_ref         0.0903
_reflns_Friedel_coverage         0.000
_reflns_number_gt                110
_reflns_number_total             114
_reflns_threshold_expression     'I > 2σ(I)'
_cod_data_source_file            cg5b00390_si_002.cif
_cod_data_source_block           marseno_012
_cod_depositor_comments
;

2022-02-23
Space group name changed to comply with IUCR recomendations
                 miguel
;
_cod_original_cell_volume        1120.87(9)
_cod_database_code               4513572
_shelx_space_group_comment
;
The symmetry employed for this shelxl refinement is uniquely defined
by the following loop, which should always be used as a source of
symmetry information in preference to the above space-group names.
They are only intended as comments.
;
_olex2_refinement_description
;
;
_shelx_shelxl_version_number     2014/7
loop_
_space_group_symop_operation_xyz
'x, y, z'
'-x+3/4, -y+1/4, z+1/2'
'-x+1/4, y+1/2, -z+3/4'
'x+1/2, -y+3/4, -z+1/4'
'z, x, y'
'z+1/2, -x+3/4, -y+1/4'
'-z+3/4, -x+1/4, y+1/2'
'-z+1/4, x+1/2, -y+3/4'
'y, z, x'
'-y+1/4, z+1/2, -x+3/4'
'y+1/2, -z+3/4, -x+1/4'
'-y+3/4, -z+1/4, x+1/2'
'y+3/4, x+1/4, -z+1/2'
'-y, -x, -z'
'y+1/4, -x+1/2, z+3/4'
'-y+1/2, x+3/4, z+1/4'
'x+3/4, z+1/4, -y+1/2'
'-x+1/2, z+3/4, y+1/4'
'-x, -z, -y'
'x+1/4, -z+1/2, y+3/4'
'z+3/4, y+1/4, -x+1/2'
'z+1/4, -y+1/2, x+3/4'
'-z+1/2, y+3/4, x+1/4'
'-z, -y, -x'
'x, y+1/2, z+1/2'
'-x+3/4, -y+3/4, z+1'
'-x+1/4, y+1, -z+5/4'
'x+1/2, -y+5/4, -z+3/4'
'z, x+1/2, y+1/2'
'z+1/2, -x+5/4, -y+3/4'
'-z+3/4, -x+3/4, y+1'
'-z+1/4, x+1, -y+5/4'
'y, z+1/2, x+1/2'
'-y+1/4, z+1, -x+5/4'
'y+1/2, -z+5/4, -x+3/4'
'-y+3/4, -z+3/4, x+1'
'y+3/4, x+3/4, -z+1'
'-y, -x+1/2, -z+1/2'
'y+1/4, -x+1, z+5/4'
'-y+1/2, x+5/4, z+3/4'
'x+3/4, z+3/4, -y+1'
'-x+1/2, z+5/4, y+3/4'
'-x, -z+1/2, -y+1/2'
'x+1/4, -z+1, y+5/4'
'z+3/4, y+3/4, -x+1'
'z+1/4, -y+1, x+5/4'
'-z+1/2, y+5/4, x+3/4'
'-z, -y+1/2, -x+1/2'
'x+1/2, y, z+1/2'
'-x+5/4, -y+1/4, z+1'
'-x+3/4, y+1/2, -z+5/4'
'x+1, -y+3/4, -z+3/4'
'z+1/2, x, y+1/2'
'z+1, -x+3/4, -y+3/4'
'-z+5/4, -x+1/4, y+1'
'-z+3/4, x+1/2, -y+5/4'
'y+1/2, z, x+1/2'
'-y+3/4, z+1/2, -x+5/4'
'y+1, -z+3/4, -x+3/4'
'-y+5/4, -z+1/4, x+1'
'y+5/4, x+1/4, -z+1'
'-y+1/2, -x, -z+1/2'
'y+3/4, -x+1/2, z+5/4'
'-y+1, x+3/4, z+3/4'
'x+5/4, z+1/4, -y+1'
'-x+1, z+3/4, y+3/4'
'-x+1/2, -z, -y+1/2'
'x+3/4, -z+1/2, y+5/4'
'z+5/4, y+1/4, -x+1'
'z+3/4, -y+1/2, x+5/4'
'-z+1, y+3/4, x+3/4'
'-z+1/2, -y, -x+1/2'
'x+1/2, y+1/2, z'
'-x+5/4, -y+3/4, z+1/2'
'-x+3/4, y+1, -z+3/4'
'x+1, -y+5/4, -z+1/4'
'z+1/2, x+1/2, y'
'z+1, -x+5/4, -y+1/4'
'-z+5/4, -x+3/4, y+1/2'
'-z+3/4, x+1, -y+3/4'
'y+1/2, z+1/2, x'
'-y+3/4, z+1, -x+3/4'
'y+1, -z+5/4, -x+1/4'
'-y+5/4, -z+3/4, x+1/2'
'y+5/4, x+3/4, -z+1/2'
'-y+1/2, -x+1/2, -z'
'y+3/4, -x+1, z+3/4'
'-y+1, x+5/4, z+1/4'
'x+5/4, z+3/4, -y+1/2'
'-x+1, z+5/4, y+1/4'
'-x+1/2, -z+1/2, -y'
'x+3/4, -z+1, y+3/4'
'z+5/4, y+3/4, -x+1/2'
'z+3/4, -y+1, x+3/4'
'-z+1, y+5/4, x+1/4'
'-z+1/2, -y+1/2, -x'
'-x, -y, -z'
'x-3/4, y-1/4, -z-1/2'
'x-1/4, -y-1/2, z-3/4'
'-x-1/2, y-3/4, z-1/4'
'-z, -x, -y'
'-z-1/2, x-3/4, y-1/4'
'z-3/4, x-1/4, -y-1/2'
'z-1/4, -x-1/2, y-3/4'
'-y, -z, -x'
'y-1/4, -z-1/2, x-3/4'
'-y-1/2, z-3/4, x-1/4'
'y-3/4, z-1/4, -x-1/2'
'-y-3/4, -x-1/4, z-1/2'
'y, x, z'
'-y-1/4, x-1/2, -z-3/4'
'y-1/2, -x-3/4, -z-1/4'
'-x-3/4, -z-1/4, y-1/2'
'x-1/2, -z-3/4, -y-1/4'
'x, z, y'
'-x-1/4, z-1/2, -y-3/4'
'-z-3/4, -y-1/4, x-1/2'
'-z-1/4, y-1/2, -x-3/4'
'z-1/2, -y-3/4, -x-1/4'
'z, y, x'
'-x, -y+1/2, -z+1/2'
'x-3/4, y+1/4, -z'
'x-1/4, -y, z-1/4'
'-x-1/2, y-1/4, z+1/4'
'-z, -x+1/2, -y+1/2'
'-z-1/2, x-1/4, y+1/4'
'z-3/4, x+1/4, -y'
'z-1/4, -x, y-1/4'
'-y, -z+1/2, -x+1/2'
'y-1/4, -z, x-1/4'
'-y-1/2, z-1/4, x+1/4'
'y-3/4, z+1/4, -x'
'-y-3/4, -x+1/4, z'
'y, x+1/2, z+1/2'
'-y-1/4, x, -z-1/4'
'y-1/2, -x-1/4, -z+1/4'
'-x-3/4, -z+1/4, y'
'x-1/2, -z-1/4, -y+1/4'
'x, z+1/2, y+1/2'
'-x-1/4, z, -y-1/4'
'-z-3/4, -y+1/4, x'
'-z-1/4, y, -x-1/4'
'z-1/2, -y-1/4, -x+1/4'
'z, y+1/2, x+1/2'
'-x+1/2, -y, -z+1/2'
'x-1/4, y-1/4, -z'
'x+1/4, -y-1/2, z-1/4'
'-x, y-3/4, z+1/4'
'-z+1/2, -x, -y+1/2'
'-z, x-3/4, y+1/4'
'z-1/4, x-1/4, -y'
'z+1/4, -x-1/2, y-1/4'
'-y+1/2, -z, -x+1/2'
'y+1/4, -z-1/2, x-1/4'
'-y, z-3/4, x+1/4'
'y-1/4, z-1/4, -x'
'-y-1/4, -x-1/4, z'
'y+1/2, x, z+1/2'
'-y+1/4, x-1/2, -z-1/4'
'y, -x-3/4, -z+1/4'
'-x-1/4, -z-1/4, y'
'x, -z-3/4, -y+1/4'
'x+1/2, z, y+1/2'
'-x+1/4, z-1/2, -y-1/4'
'-z-1/4, -y-1/4, x'
'-z+1/4, y-1/2, -x-1/4'
'z, -y-3/4, -x+1/4'
'z+1/2, y, x+1/2'
'-x+1/2, -y+1/2, -z'
'x-1/4, y+1/4, -z-1/2'
'x+1/4, -y, z-3/4'
'-x, y-1/4, z-1/4'
'-z+1/2, -x+1/2, -y'
'-z, x-1/4, y-1/4'
'z-1/4, x+1/4, -y-1/2'
'z+1/4, -x, y-3/4'
'-y+1/2, -z+1/2, -x'
'y+1/4, -z, x-3/4'
'-y, z-1/4, x-1/4'
'y-1/4, z+1/4, -x-1/2'
'-y-1/4, -x+1/4, z-1/2'
'y+1/2, x+1/2, z'
'-y+1/4, x, -z-3/4'
'y, -x-1/4, -z-1/4'
'-x-1/4, -z+1/4, y-1/2'
'x, -z-1/4, -y-1/4'
'x+1/2, z+1/2, y'
'-x+1/4, z, -y-3/4'
'-z-1/4, -y+1/4, x-1/2'
'-z+1/4, y, -x-3/4'
'z, -y-1/4, -x-1/4'
'z+1/2, y+1/2, x'
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_site_symmetry_order
_atom_site_calc_flag
_atom_site_refinement_flags_posn
_atom_site_refinement_flags_adp
_atom_site_refinement_flags_occupancy
As1 As 0.26453(5) 0.26453(5) 0.26453(5) 0.0097(4) Uani 1 6 d S T P
O1 O 0.3750 0.3750 0.1910(4) 0.0095(9) Uani 1 4 d S T P
loop_
_atom_type_symbol
_atom_type_description
_atom_type_scat_dispersion_real
_atom_type_scat_dispersion_imag
_atom_type_scat_source
As As 0.3110 0.7990 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'
O O 0.0020 0.0020 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'
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
O1 As1 O1 97.78(18) . 9
O1 As1 O1 97.78(18) 9 5
O1 As1 O1 97.78(18) . 5
As1 O1 As1 129.6(3) . 26_554
loop_
_geom_bond_atom_site_label_1
_geom_bond_atom_site_label_2
_geom_bond_distance
_geom_bond_site_symmetry_2
As1 O1 1.793(2) .
As1 O1 1.794(2) 5
As1 O1 1.794(2) 9
O1 As1 1.794(2) 26_554
