                     θ~max~ = 00.0°, θ~min~ = 0.0°   ω scans                                                      *h* = −00→00   Absorption correction: multi-scan (*SADABS*; Bruker, 0000)   *k* = −00→00   *T*~min~ = 0.000, *T*~max~ = 0.000                           *l* = −00→00   00000 measured reflections                                      ------------------------------------------------------------ --------------------------------------  Refinement {#tablewraprefinementdatalong} ==========    ------------------------------------- -------------------------------------------------------------------------------------   Refinement on *F*^0^                  Primary atom site location: structure-invariant direct methods   Least-squares matrix: full            Secondary atom site location: difference Fourier map   *R*\[*F*^0^ \> 0σ(*F*^0^)\] = 0.000   Hydrogen site location: inferred from neighbouring sites   *wR*(*F*^0^) = 0.000                  H-atom parameters constrained   *S* = 0.00                            *w* = 0/\[σ^0^(*F*~o~^0^) + (0.0000*P*)^0^\] where *P* = (*F*~o~^0^ + 0*F*~c~^0^)/0   0000 reflections                      (Δ/σ)~max~ \< 0.000   000 parameters                        Δρ~max~ = 0.00 e Å^−0^   0 restraints                          Δρ~min~ = −0.00 e Å^−0^   ------------------------------------- -------------------------------------------------------------------------------------  Special details {#specialdetails} ===============    ----------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------   Geometry. All s.u.\'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.\'s are taken into account individually in the estimation of s.u.\'s in distances, angles and torsion angles; correlations between s.u.\'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.\'s is used for estimating s.u.\'s involving l.s. planes.   Refinement. Refinement of *F*^0^ against ALL reflections. The weighted *R*-factor *wR* and goodness of fit *S* are based on *F*^0^, conventional *R*-factors *R* are based on *F*, with *F* set to zero for negative *F*^0^. The threshold expression of *F*^0^ \> σ(*F*^0^) 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*^0^ are statistically about twice as large as those based on *F*, and *R*-factors based on ALL data will be even larger.   ----------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------  Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å^0^) {#tablewrapcoords} ==================================================================================================    ------ -------------- --------------- -------------- -------------------- --          *x*            *y*             *z*            *U*~iso~\*/*U*~eq~      Cl0    0.00000 (0