A %(colour)s %(shape)s-shaped crystal with dimensions %(crystal_size)s mm<sup>3</sup> was %(mounting)s. Data were collected using an %(diffractometer)s diffractometer %(olex2_diffrn_ambient_temperature_device)s at %(cell_measurement_temperature)s.

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Data were measured %(runs)s using %(radiation)s radiation. %(strategy)s The maximum resolution that was achieved was &Theta; = %(_diffrn_reflns_theta_max)sDEGREES %(min_d_full)s

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The diffraction pattern was indexed %(indexing)s and the unit cell was refined %(cell_refine)s on %(_cell_measurement_reflns_used)s reflections, %(cell_reflections_percentage)sPERCENT of the observed reflections.

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Data reduction, scaling and absorption corrections were performed %(data_reduction)s. The final completeness is %(_diffrn_measured_fraction_theta_full_percentage)s PERCENT out to %(_diffrn_reflns_theta_max)sDEGREES in &Theta;. %(absorption_correction)s.

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The structure was solved and the space group %(sg)s (HASH %(space_group_IT_number)s) determined by the %(_computing_structure_solution)s structure solution program using %(solution_method)s and refined by %(refinement_method)s using %(_shelxl_version_number)s %(_computing_structure_refinement)s. All non-hydrogen atoms were refined anisotropically. Hydrogen atom positions were calculated geometrically and refined using the riding model. 

%(refine_ls_hydrogen_treatment)s