One-dimensional magnetic halide double perovskites [N(CH<sub>3</sub>)<sub>4</sub>]<sub>2</sub>M<sup>I</sup>MoCl<sub>6</sub> (M<sup>I</sup> = Na, Ag) with large A-site cations.
Binwal, Devesh Chandra; Vishnoi, Pratap; Chemical communications (Cambridge, England) 61 (2025) 18352–18355; doi:10.1039/d5cc04751j

data_7135085
_publ_section_title
;
 One-dimensional magnetic halide double perovskites
 [N(CH<sub>3</sub>)<sub>4</sub>]<sub>2</sub>M<sup>I</sup>MoCl<sub>6</sub>
 (M<sup>I</sup> = Na, Ag) with large A-site cations.
;
_journal_issue                   93
_journal_name_full               'Chemical communications (Cambridge, England)'
_journal_page_first              18352
_journal_page_last               18355
_journal_paper_doi               10.1039/d5cc04751j
_journal_volume                  61
_journal_year                    2025
_chemical_formula_moiety         C8H24AgCl6MoN2
_chemical_formula_sum            'C8 H24 Ag Cl6 Mo N2'
_chemical_formula_weight         564.81
_space_group_crystal_system      hexagonal
_space_group_IT_number           194
_space_group_name_Hall           '-P 6c 2c'
_space_group_name_H-M_alt        'P 63/m m c'
_atom_sites_solution_hydrogens   geom
_atom_sites_solution_primary     'Intrinsic Phasing'
_audit_creation_method
;FinalCif 2025.6-RC13 by Daniel Kratzert, Freiburg 2025, 
https://dkratzert.de/finalcif.html
;
_audit_update_record
;
2025-10-13 deposited with the CCDC.	2025-10-16 downloaded from the CCDC.
;
_cell_angle_alpha                90
_cell_angle_beta                 90
_cell_angle_gamma                120
_cell_formula_units_Z            1
_cell_length_a                   9.0540(8)
_cell_length_b                   9.0540(8)
_cell_length_c                   6.7638(10)
_cell_measurement_reflns_used    3374
_cell_measurement_temperature    300(2)
_cell_measurement_theta_max      25.61
_cell_measurement_theta_min      2.6
_cell_measurement_wavelength     0.71073
_cell_volume                     480.18(9)
_computing_cell_refinement       'SAINT V8.41 (Bruker AXS LLC)'
_computing_data_collection
'Bruker Instrument Service, BIS, v.6.2.12 (Bruker AXS Inc., 2023)'
_computing_data_reduction        'SAINT V8.41 (Bruker AXS LLC)'
_computing_molecular_graphics    'shelXle (C.B. Huebschle, rev 1773)'
_computing_publication_material  'Bruker SHELXTL'
_computing_structure_refinement  'SHELXL-2019/2 (Sheldrick, 2019)'
_computing_structure_solution    'SHELXT 2014/5 (Sheldrick, 2014)'
_diffrn_ambient_environment      N~2~
_diffrn_ambient_temperature      300(2)
_diffrn_detector                 CPAD
_diffrn_detector_type            'Bruker PHOTON II'
_diffrn_measured_fraction_theta_full 1.000
_diffrn_measured_fraction_theta_max 1.000
_diffrn_measurement_device       'KAPPA diffractometer'
_diffrn_measurement_device_type  'Bruker D8 VENTURE'
_diffrn_measurement_method       '\w and \f scans'
_diffrn_radiation_monochromator  'multilayer mirror'
_diffrn_radiation_probe          x-ray
_diffrn_radiation_type           MoK\a
_diffrn_radiation_wavelength     0.71073
_diffrn_reflns_av_R_equivalents  0.1418
_diffrn_reflns_av_unetI/netI     0.0198
_diffrn_reflns_Laue_measured_fraction_full 1.000
_diffrn_reflns_Laue_measured_fraction_max 1.000
_diffrn_reflns_limit_h_max       10
_diffrn_reflns_limit_h_min       -11
_diffrn_reflns_limit_k_max       11
_diffrn_reflns_limit_k_min       -11
_diffrn_reflns_limit_l_max       8
_diffrn_reflns_limit_l_min       -8
_diffrn_reflns_number            12457
_diffrn_reflns_point_group_measured_fraction_full 1.000
_diffrn_reflns_point_group_measured_fraction_max 1.000
_diffrn_reflns_theta_full        25.242
_diffrn_reflns_theta_max         27.037
_diffrn_reflns_theta_min         2.598
_diffrn_source                   'microfocus sealed tube'
_diffrn_source_current           1.0
_diffrn_source_type              'INCOATEC I\mS 3.0'
_diffrn_source_voltage           50
_exptl_absorpt_coefficient_mu    2.491
_exptl_absorpt_correction_T_max  0.771
_exptl_absorpt_correction_T_min  0.662
_exptl_absorpt_correction_type   multi-scan
_exptl_absorpt_process_details
;Krause, L., Herbst-Irmer, R., Sheldrick, G. M., Stalke, D. (2015).
"Comparison of silver and molybdenum microfocus X-ray sources for single-crystal
 structure determination"
J. Appl. Cryst. 48, 3-10.
doi:10.1107/S1600576714022985
;
_exptl_crystal_colour            red
_exptl_crystal_density_diffrn    1.953
_exptl_crystal_description       plate
_exptl_crystal_F_000             277
_exptl_crystal_size_max          0.18
_exptl_crystal_size_mid          0.15
_exptl_crystal_size_min          0.11
_refine_diff_density_max         0.782
_refine_diff_density_min         -0.785
_refine_diff_density_rms         0.113
_refine_ls_extinction_method     none
_refine_ls_goodness_of_fit_ref   1.178
_refine_ls_hydrogen_treatment    constr
_refine_ls_matrix_type           full
_refine_ls_number_parameters     29
_refine_ls_number_reflns         232
_refine_ls_number_restraints     16
_refine_ls_restrained_S_all      1.144
_refine_ls_R_factor_all          0.0587
_refine_ls_R_factor_gt           0.0508
_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/[\s^2^(Fo^2^)+4.8798P] where P=(Fo^2^+2Fc^2^)/3'
_refine_ls_weighting_scheme      calc
_refine_ls_wR_factor_gt          0.1019
_refine_ls_wR_factor_ref         0.1067
_reflns_Friedel_coverage         0.000
_reflns_number_gt                200
_reflns_number_total             232
_reflns_threshold_expression     'I > 2\s(I)'
_cod_data_source_file            d5cc04751j2.cif
_cod_data_source_block           TMA2AgMoCl6
_cod_depositor_comments
'Adding full bibliography for 7135084--7135085.cif.'
_cod_original_cell_volume        480.18(11)
_cod_database_code               7135085
_shelx_shelxl_version_number     2019/3
_shelx_estimated_absorpt_t_min   0.662
_shelx_estimated_absorpt_t_max   0.771
_bruker_diffrn_measurement_temperature_device 'Oxford Cryostream 1000'
_geom_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.
;
_shelx_res_checksum              34823
_shelx_hkl_checksum              20349