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The polyfluorinated title compounds, [MBr2(C18H16F8N2O2)] or [4,4′-(HCF2CF2CH2OCH2)2-2,2′-bpy]MBr2, (1) (M = Pd and bpy is bipyridine) and (2) (M = Pt), have –CH(α)2OCH(β)2CF2CF2H side chains with methyl­ene H-atom donors at the α and β sites, and methine H-atom donors at the terminal sites, in addition to aromatic H-atom donors. In contrast to the original expectation of iso­morphous structures, (1) crystallizes in the space group C2/c and (2) in P21/n, with similar unit-cell volumes and Z = 4. The asymmetric unit of (1) is one half of the mol­ecule, which resides on a crystallographic twofold axis. Both (1) and (2) display stacking of the mol­ecules, indicating a planar (bpy)MBr2 skeleton in each case. The structure of (1) exhibits columns with C—H(β)...Br hydrogen bonds between consecutive layers which conforms to a static (β,β) linkage between layers. In the mol­ecular plane, (1) shows double C—H(α)...Br hydrogen bonds self-repeating along the b axis, the planar molecules being connected into infinite belts. Compound (2) has no crystallographic symmetry and forms π-dimer pairs as supermolecules, which then stack parallel to the a axis. The π-dimer-pair super­molecules exhibit (Pt—)Br...Br(—Pt) contacts [3.6937 (7) Å] to neighbouring π-dimer pairs crosslinking the columns. The structure of (2) reveals many C—H...F(—C) inter­actions between F atoms and aromatic C—H groups, in addition to those between F atoms and methyl­ene C—H groups.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229618005715/ku3214sup1.cif
Contains datablocks i12782, i15498, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229618005715/ku3214i12782sup2.hkl
Contains datablock i12782

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229618005715/ku3214i15498sup3.hkl
Contains datablock i15498

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2053229618005715/ku3214sup4.pdf
Additional figure and fingerprint plots

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229618005715/ku3214sup5.cif
Data for (2) at 295 K

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229618005715/ku3214sup6.cif
Data for (1) at 293 K

CCDC references: 1836458; 1836457

Computing details top

Data collection: APEX3 (Bruker, 2015) for i12782; APEX2 (Bruker, 2015) for i15498. Cell refinement: APEX3 (Bruker, 2015) for i12782; SAINT (Bruker, 2015) for i15498. For both structures, data reduction: SAINT (Bruker, 2015). Program(s) used to solve structure: SHELXT (Sheldrick, 2015a) for i12782; SHELXS97 (Sheldrick, 2008) for i15498. For both structures, program(s) used to refine structure: SHELXL2013 (Sheldrick, 2015b). Molecular graphics: shelXle (Hübschle et al., 2011) for i12782; SHELXTL (Sheldrick, 2008) for i15498. Software used to prepare material for publication: WinGX (Farrugia, 2012) and Mercury (Macrae et al., 2008) for i12782; SHELXTL (Sheldrick, 2008) and Mercury (Macrae et al., 2008) for i15498.

{4,4'-Bis[(2,2,3,3-tetrafluoropropoxy)methyl]-2,2'-bipyridine-κ2N,N'}dibromidopalladium (i12782) top
Crystal data top
[PdBr2(C18H16F8N2O2)]F(000) = 1368
Mr = 710.55Dx = 2.114 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
a = 24.0989 (7) ÅCell parameters from 8599 reflections
b = 9.7107 (3) Åθ = 2.3–26.4°
c = 9.5630 (3) ŵ = 4.50 mm1
β = 93.819 (2)°T = 295 K
V = 2232.94 (12) Å3Prism, orange
Z = 40.18 × 0.16 × 0.14 mm
Data collection top
Bruker APEXII CCD
diffractometer
2062 reflections with I > 2σ(I)
φ and ω scansRint = 0.024
Absorption correction: multi-scan
(SADABS; Bruker, 2015)
θmax = 26.4°, θmin = 2.3°
Tmin = 0.618, Tmax = 0.745h = 3028
19843 measured reflectionsk = 1112
2275 independent reflectionsl = 1111
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.026H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.067 w = 1/[σ2(Fo2) + (0.0334P)2 + 6.1015P]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max < 0.001
2275 reflectionsΔρmax = 0.73 e Å3
153 parametersΔρmin = 0.72 e Å3
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Pd10.5000000.31069 (3)0.7500000.02942 (10)
Br10.45416 (2)0.13376 (3)0.60961 (4)0.04608 (12)
F10.25678 (11)0.9736 (4)0.1191 (3)0.0964 (11)
F20.28718 (14)0.7675 (5)0.1241 (4)0.1429 (19)
F30.20657 (14)0.9294 (7)0.3492 (5)0.178 (3)
F40.18172 (12)0.7861 (4)0.1882 (4)0.1008 (11)
O10.33803 (9)0.8051 (2)0.3838 (2)0.0433 (5)
N10.46099 (9)0.4704 (2)0.6461 (2)0.0284 (5)
C20.47739 (10)0.5974 (3)0.6933 (3)0.0251 (5)
C30.45311 (10)0.7156 (3)0.6391 (3)0.0263 (5)
H30.4645620.8010780.6740290.032*
C40.41104 (11)0.7067 (3)0.5312 (3)0.0280 (6)
C50.39553 (11)0.5775 (3)0.4837 (3)0.0331 (6)
H50.3680650.5678590.4113200.040*
C60.42071 (11)0.4629 (3)0.5434 (3)0.0333 (6)
H60.4092530.3765210.5110160.040*
C70.38622 (12)0.8361 (3)0.4717 (3)0.0329 (6)
H7A0.3763700.8964020.5470590.039*
H7B0.4131430.8835600.4180210.039*
C80.32082 (13)0.9193 (4)0.3009 (3)0.0440 (7)
H8A0.3507690.9505140.2458590.053*
H8B0.3098760.9946860.3597040.053*
C90.27238 (15)0.8717 (4)0.2070 (4)0.0532 (9)
C100.2238 (2)0.8236 (6)0.2794 (5)0.0779 (15)
H100.224 (2)0.770 (6)0.359 (6)0.093*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pd10.02884 (16)0.01931 (16)0.04132 (18)0.0000.01131 (12)0.000
Br10.0480 (2)0.02557 (18)0.0661 (2)0.00933 (12)0.01380 (16)0.01196 (14)
F10.0716 (16)0.136 (3)0.0766 (17)0.0089 (17)0.0283 (13)0.0629 (18)
F20.106 (2)0.215 (4)0.100 (2)0.077 (3)0.054 (2)0.109 (3)
F30.074 (2)0.326 (8)0.139 (3)0.069 (3)0.052 (2)0.135 (5)
F40.0662 (17)0.108 (2)0.121 (2)0.0232 (16)0.0456 (17)0.0030 (19)
O10.0409 (12)0.0381 (12)0.0477 (12)0.0027 (9)0.0208 (10)0.0040 (10)
N10.0254 (11)0.0254 (12)0.0352 (12)0.0029 (9)0.0066 (9)0.0052 (10)
C20.0238 (12)0.0249 (13)0.0272 (12)0.0025 (10)0.0058 (10)0.0014 (10)
C30.0255 (12)0.0240 (13)0.0293 (12)0.0020 (10)0.0007 (10)0.0021 (10)
C40.0244 (12)0.0320 (15)0.0276 (12)0.0000 (10)0.0024 (10)0.0031 (11)
C50.0274 (13)0.0387 (16)0.0324 (14)0.0047 (12)0.0028 (11)0.0073 (12)
C60.0301 (14)0.0301 (15)0.0396 (15)0.0052 (11)0.0020 (11)0.0097 (12)
C70.0311 (14)0.0334 (15)0.0329 (14)0.0000 (12)0.0071 (11)0.0023 (12)
C80.0383 (16)0.053 (2)0.0401 (16)0.0023 (15)0.0049 (13)0.0124 (15)
C90.049 (2)0.071 (3)0.0371 (17)0.0148 (18)0.0084 (15)0.0021 (16)
C100.063 (3)0.098 (4)0.069 (3)0.030 (3)0.019 (2)0.013 (3)
Geometric parameters (Å, º) top
Pd1—N12.038 (2)C3—C41.401 (3)
Pd1—N1i2.038 (2)C3—H30.9300
Pd1—Br12.4035 (4)C4—C51.378 (4)
Pd1—Br1i2.4035 (4)C4—C71.489 (4)
F1—C91.337 (4)C5—C61.373 (4)
F2—C91.348 (5)C5—H50.9300
F3—C101.308 (8)C6—H60.9300
F4—C101.343 (5)C7—H7A0.9700
O1—C81.409 (4)C7—H7B0.9700
O1—C71.420 (3)C8—C91.498 (5)
N1—C61.336 (4)C8—H8A0.9700
N1—C21.363 (3)C8—H8B0.9700
C2—C31.373 (4)C9—C101.475 (6)
C2—C2i1.486 (5)C10—H100.92 (6)
N1—Pd1—N1i80.86 (13)O1—C7—C4109.8 (2)
N1—Pd1—Br195.27 (6)O1—C7—H7A109.7
N1i—Pd1—Br1175.13 (6)C4—C7—H7A109.7
N1—Pd1—Br1i175.13 (6)O1—C7—H7B109.7
N1i—Pd1—Br1i95.27 (6)C4—C7—H7B109.7
Br1—Pd1—Br1i88.75 (2)H7A—C7—H7B108.2
C8—O1—C7111.4 (2)O1—C8—C9106.4 (3)
C6—N1—C2118.2 (2)O1—C8—H8A110.4
C6—N1—Pd1127.30 (19)C9—C8—H8A110.4
C2—N1—Pd1114.42 (18)O1—C8—H8B110.4
N1—C2—C3121.6 (2)C9—C8—H8B110.4
N1—C2—C2i115.09 (15)H8A—C8—H8B108.6
C3—C2—C2i123.27 (15)F1—C9—F2105.0 (3)
C2—C3—C4119.7 (3)F1—C9—C10109.3 (3)
C2—C3—H3120.1F2—C9—C10106.8 (4)
C4—C3—H3120.1F1—C9—C8108.9 (3)
C5—C4—C3117.8 (3)F2—C9—C8111.0 (3)
C5—C4—C7123.3 (2)C10—C9—C8115.3 (3)
C3—C4—C7118.9 (2)F3—C10—F4107.0 (5)
C6—C5—C4119.9 (2)F3—C10—C9106.2 (5)
C6—C5—H5120.1F4—C10—C9111.7 (4)
C4—C5—H5120.1F3—C10—H1090 (4)
N1—C6—C5122.7 (3)F4—C10—H10110 (3)
N1—C6—H6118.6C9—C10—H10127 (3)
C5—C6—H6118.6
C6—N1—C2—C30.9 (4)C8—O1—C7—C4166.4 (3)
Pd1—N1—C2—C3176.7 (2)C5—C4—C7—O112.2 (4)
C6—N1—C2—C2i179.6 (3)C3—C4—C7—O1169.1 (2)
Pd1—N1—C2—C2i2.9 (3)C7—O1—C8—C9176.5 (3)
N1—C2—C3—C41.1 (4)O1—C8—C9—F1175.7 (3)
C2i—C2—C3—C4179.4 (3)O1—C8—C9—F260.6 (4)
C2—C3—C4—C50.2 (4)O1—C8—C9—C1061.0 (5)
C2—C3—C4—C7178.6 (2)F1—C9—C10—F361.0 (5)
C3—C4—C5—C60.8 (4)F2—C9—C10—F3174.2 (4)
C7—C4—C5—C6179.5 (3)C8—C9—C10—F362.0 (6)
C2—N1—C6—C50.2 (4)F1—C9—C10—F455.3 (6)
Pd1—N1—C6—C5177.4 (2)F2—C9—C10—F457.8 (5)
C4—C5—C6—N11.1 (4)C8—C9—C10—F4178.4 (4)
Symmetry code: (i) x+1, y, z+3/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C5—H5···O10.932.422.746 (3)100
C6—H6···Br10.932.733.346 (3)124
C7—H7A···Br1ii0.973.013.534 (3)116
C8—H8A···Br1iii0.973.003.837 (3)145
Symmetry codes: (ii) x, y+1, z; (iii) x, y+1, z1/2.
{4,4'-Bis[(2,2,3,3-tetrafluoropropoxy)methyl]-2,2'-bipyridine-κ2N,N'}dibromidoplatinum (i15498) top
Crystal data top
[PtBr2(C18H16F8N2O2)]F(000) = 1496
Mr = 799.24Dx = 2.472 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 6.9344 (3) ÅCell parameters from 9815 reflections
b = 11.8500 (5) Åθ = 2.3–27.2°
c = 26.3196 (12) ŵ = 10.34 mm1
β = 96.766 (2)°T = 100 K
V = 2147.69 (16) Å3Plate, yellow
Z = 40.12 × 0.08 × 0.06 mm
Data collection top
Bruker APEXII CCD
diffractometer
4462 reflections with I > 2σ(I)
φ and ω scansRint = 0.041
Absorption correction: multi-scan
(SADABS; Bruker, 2015)
θmax = 27.1°, θmin = 1.9°
Tmin = 0.592, Tmax = 0.971h = 88
77853 measured reflectionsk = 1515
4733 independent reflectionsl = 3333
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.023Only H-atom coordinates refined
wR(F2) = 0.059 w = 1/[σ2(Fo2) + (0.0146P)2 + 15.9277P]
where P = (Fo2 + 2Fc2)/3
S = 1.20(Δ/σ)max = 0.001
4733 reflectionsΔρmax = 1.26 e Å3
346 parametersΔρmin = 0.99 e Å3
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Pt10.17097 (2)0.66847 (2)0.46257 (2)0.00863 (5)
Br10.08580 (6)0.86348 (4)0.47733 (2)0.01307 (9)
Br20.13801 (7)0.70814 (4)0.37189 (2)0.01582 (10)
F10.4760 (5)0.0003 (3)0.32226 (12)0.0360 (9)
F20.7463 (5)0.0793 (3)0.35482 (13)0.0320 (8)
F30.6165 (5)0.2007 (2)0.37112 (13)0.0262 (7)
F40.7671 (5)0.1303 (3)0.31023 (11)0.0257 (7)
F50.3600 (4)0.3124 (2)0.76645 (11)0.0187 (6)
F60.6122 (4)0.3424 (3)0.82330 (10)0.0212 (6)
F70.6045 (5)0.1398 (3)0.77658 (12)0.0302 (7)
F80.8486 (5)0.2464 (3)0.76164 (14)0.0346 (8)
O10.4694 (5)0.1250 (3)0.41236 (13)0.0177 (7)
O20.5064 (5)0.4550 (3)0.69661 (12)0.0170 (7)
N10.2415 (5)0.5037 (3)0.45526 (14)0.0094 (7)
N20.2043 (5)0.6225 (3)0.53767 (14)0.0103 (7)
C10.2731 (6)0.4464 (4)0.50052 (17)0.0096 (8)
C20.3204 (6)0.3327 (4)0.50151 (17)0.0115 (8)
H20.338 (7)0.289 (5)0.534 (2)0.014*
C30.3368 (6)0.2753 (4)0.45611 (17)0.0106 (8)
C40.3070 (6)0.3353 (4)0.41027 (18)0.0130 (9)
H40.312 (8)0.304 (5)0.380 (2)0.016*
C50.2591 (6)0.4488 (4)0.41165 (18)0.0127 (9)
H50.240 (8)0.491 (5)0.385 (2)0.015*
C60.2558 (6)0.5133 (4)0.54633 (17)0.0106 (8)
C70.2881 (6)0.4714 (4)0.59569 (18)0.0124 (9)
H70.319 (8)0.397 (5)0.599 (2)0.015*
C80.2712 (6)0.5416 (4)0.63697 (17)0.0135 (9)
C90.2185 (7)0.6530 (4)0.62751 (18)0.0141 (9)
H90.205 (8)0.706 (5)0.652 (2)0.017*
C100.1857 (6)0.6909 (4)0.57768 (17)0.0108 (8)
H100.161 (8)0.771 (5)0.573 (2)0.013*
C110.3895 (7)0.1525 (4)0.45747 (18)0.0134 (9)
H11A0.477 (8)0.129 (5)0.487 (2)0.016*
H11B0.280 (8)0.111 (5)0.461 (2)0.016*
C120.5364 (7)0.0127 (4)0.41185 (18)0.0134 (9)
H12A0.436 (8)0.039 (5)0.415 (2)0.016*
H12B0.646 (8)0.005 (5)0.443 (2)0.016*
C130.6195 (7)0.0038 (4)0.36220 (17)0.0147 (9)
C140.7309 (7)0.1145 (4)0.35903 (18)0.0159 (9)
H140.841 (9)0.111 (5)0.378 (2)0.019*
C150.3119 (7)0.4980 (5)0.69104 (18)0.0176 (10)
H15A0.303 (8)0.556 (5)0.716 (2)0.021*
H15B0.219 (8)0.443 (5)0.698 (2)0.021*
C160.5938 (8)0.4476 (4)0.74773 (19)0.0195 (10)
H16A0.555 (9)0.503 (5)0.773 (2)0.023*
H16B0.734 (9)0.458 (5)0.747 (2)0.023*
C170.5543 (7)0.3354 (4)0.77188 (17)0.0162 (9)
C180.6537 (7)0.2341 (5)0.7512 (2)0.0202 (10)
H180.629 (8)0.214 (5)0.715 (2)0.024*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pt10.00835 (8)0.00805 (8)0.00931 (8)0.00030 (6)0.00037 (5)0.00083 (6)
Br10.0166 (2)0.0082 (2)0.0141 (2)0.00190 (16)0.00047 (16)0.00065 (16)
Br20.0218 (2)0.0156 (2)0.0105 (2)0.00604 (18)0.00360 (17)0.00360 (17)
F10.045 (2)0.041 (2)0.0180 (16)0.0288 (17)0.0119 (14)0.0054 (14)
F20.052 (2)0.0134 (15)0.0366 (19)0.0031 (14)0.0292 (16)0.0005 (13)
F30.0286 (16)0.0109 (14)0.0396 (19)0.0003 (12)0.0062 (14)0.0013 (13)
F40.0375 (18)0.0262 (16)0.0134 (14)0.0138 (14)0.0033 (12)0.0044 (12)
F50.0189 (14)0.0191 (15)0.0182 (14)0.0012 (11)0.0021 (11)0.0035 (11)
F60.0299 (16)0.0219 (15)0.0104 (13)0.0034 (13)0.0033 (11)0.0001 (11)
F70.045 (2)0.0172 (16)0.0280 (17)0.0070 (14)0.0038 (15)0.0031 (13)
F80.0229 (16)0.044 (2)0.0362 (19)0.0099 (15)0.0020 (14)0.0019 (16)
O10.0244 (18)0.0128 (16)0.0163 (17)0.0069 (14)0.0045 (14)0.0021 (13)
O20.0164 (16)0.0225 (18)0.0114 (16)0.0028 (14)0.0008 (13)0.0041 (14)
N10.0083 (16)0.0104 (18)0.0094 (17)0.0002 (14)0.0002 (13)0.0030 (14)
N20.0054 (16)0.0105 (18)0.0142 (18)0.0015 (14)0.0016 (13)0.0003 (15)
C10.0064 (18)0.010 (2)0.012 (2)0.0013 (15)0.0007 (15)0.0010 (16)
C20.0076 (19)0.014 (2)0.012 (2)0.0020 (16)0.0018 (15)0.0009 (18)
C30.0074 (19)0.009 (2)0.015 (2)0.0015 (15)0.0000 (16)0.0032 (17)
C40.011 (2)0.014 (2)0.014 (2)0.0030 (17)0.0002 (16)0.0046 (18)
C50.013 (2)0.014 (2)0.011 (2)0.0001 (17)0.0013 (16)0.0019 (18)
C60.0070 (18)0.012 (2)0.012 (2)0.0019 (16)0.0009 (15)0.0011 (17)
C70.011 (2)0.011 (2)0.015 (2)0.0013 (17)0.0003 (16)0.0017 (17)
C80.011 (2)0.017 (2)0.013 (2)0.0002 (17)0.0026 (17)0.0023 (18)
C90.013 (2)0.015 (2)0.015 (2)0.0004 (17)0.0024 (17)0.0027 (18)
C100.011 (2)0.011 (2)0.010 (2)0.0008 (16)0.0018 (16)0.0003 (16)
C110.016 (2)0.009 (2)0.016 (2)0.0014 (18)0.0043 (18)0.0005 (17)
C120.016 (2)0.008 (2)0.016 (2)0.0010 (17)0.0025 (18)0.0004 (17)
C130.022 (2)0.012 (2)0.010 (2)0.0034 (18)0.0018 (17)0.0020 (17)
C140.020 (2)0.016 (2)0.011 (2)0.0005 (19)0.0004 (18)0.0010 (18)
C150.018 (2)0.022 (3)0.012 (2)0.005 (2)0.0013 (18)0.005 (2)
C160.021 (3)0.020 (3)0.015 (2)0.005 (2)0.0072 (19)0.002 (2)
C170.018 (2)0.019 (2)0.010 (2)0.0002 (19)0.0040 (17)0.0009 (18)
C180.023 (2)0.023 (3)0.015 (2)0.006 (2)0.0015 (19)0.001 (2)
Geometric parameters (Å, º) top
Pt1—N12.027 (4)C4—C51.388 (7)
Pt1—N22.037 (4)C4—H40.88 (6)
Pt1—Br22.4168 (5)C5—H50.86 (6)
Pt1—Br12.4277 (5)C6—C71.384 (6)
F1—C131.360 (5)C7—C81.384 (7)
F2—C131.350 (6)C7—H70.91 (6)
F3—C141.354 (6)C8—C91.384 (7)
F4—C141.350 (5)C8—C151.509 (6)
F5—C171.366 (6)C9—C101.380 (6)
F6—C171.368 (5)C9—H90.91 (6)
F7—C181.366 (6)C10—H100.97 (6)
F8—C181.355 (6)C11—H11A0.98 (6)
O1—C111.406 (6)C11—H11B0.92 (6)
O1—C121.410 (5)C12—C131.502 (6)
O2—C161.412 (6)C12—H12A0.94 (6)
O2—C151.433 (6)C12—H12B1.05 (6)
N1—C51.337 (6)C13—C141.529 (7)
N1—C11.366 (6)C14—H140.87 (6)
N2—C101.346 (6)C15—H15A0.96 (6)
N2—C61.355 (6)C15—H15B0.95 (6)
C1—C21.387 (6)C16—C171.512 (7)
C1—C61.460 (6)C16—H16A1.00 (6)
C2—C31.391 (6)C16—H16B0.98 (6)
C2—H21.00 (6)C17—C181.517 (7)
C3—C41.394 (6)C18—H180.98 (6)
C3—C111.500 (6)
N1—Pt1—N280.43 (15)C3—C11—H11A115 (3)
N1—Pt1—Br295.13 (10)O1—C11—H11B112 (4)
N2—Pt1—Br2175.56 (11)C3—C11—H11B109 (4)
N1—Pt1—Br1176.19 (10)H11A—C11—H11B102 (5)
N2—Pt1—Br195.79 (11)O1—C12—C13107.0 (4)
Br2—Pt1—Br188.651 (16)O1—C12—H12A112 (3)
C11—O1—C12112.9 (4)C13—C12—H12A111 (3)
C16—O2—C15114.4 (4)O1—C12—H12B107 (3)
C5—N1—C1119.0 (4)C13—C12—H12B110 (3)
C5—N1—Pt1126.7 (3)H12A—C12—H12B110 (5)
C1—N1—Pt1114.3 (3)F2—C13—F1107.0 (4)
C10—N2—C6119.4 (4)F2—C13—C12110.7 (4)
C10—N2—Pt1126.0 (3)F1—C13—C12110.3 (4)
C6—N2—Pt1114.6 (3)F2—C13—C14106.0 (4)
N1—C1—C2120.9 (4)F1—C13—C14108.5 (4)
N1—C1—C6115.4 (4)C12—C13—C14114.1 (4)
C2—C1—C6123.7 (4)F4—C14—F3107.3 (4)
C1—C2—C3120.1 (4)F4—C14—C13108.9 (4)
C1—C2—H2121 (3)F3—C14—C13108.7 (4)
C3—C2—H2119 (3)F4—C14—H14108 (4)
C2—C3—C4118.4 (4)F3—C14—H14114 (4)
C2—C3—C11119.8 (4)C13—C14—H14110 (4)
C4—C3—C11121.7 (4)O2—C15—C8106.7 (4)
C5—C4—C3118.9 (4)O2—C15—H15A109 (4)
C5—C4—H4118 (4)C8—C15—H15A112 (4)
C3—C4—H4123 (4)O2—C15—H15B113 (4)
N1—C5—C4122.7 (4)C8—C15—H15B111 (4)
N1—C5—H5114 (4)H15A—C15—H15B105 (5)
C4—C5—H5124 (4)O2—C16—C17112.1 (4)
N2—C6—C7120.7 (4)O2—C16—H16A119 (3)
N2—C6—C1115.2 (4)C17—C16—H16A103 (3)
C7—C6—C1124.1 (4)O2—C16—H16B107 (4)
C6—C7—C8120.2 (4)C17—C16—H16B110 (4)
C6—C7—H7117 (4)H16A—C16—H16B106 (5)
C8—C7—H7123 (4)F5—C17—F6106.7 (4)
C7—C8—C9118.5 (4)F5—C17—C16110.9 (4)
C7—C8—C15120.7 (4)F6—C17—C16108.4 (4)
C9—C8—C15120.8 (4)F5—C17—C18106.8 (4)
C10—C9—C8119.5 (4)F6—C17—C18108.1 (4)
C10—C9—H9116 (4)C16—C17—C18115.6 (4)
C8—C9—H9125 (4)F8—C18—F7106.8 (4)
N2—C10—C9121.8 (4)F8—C18—C17109.1 (4)
N2—C10—H10121 (3)F7—C18—C17108.7 (4)
C9—C10—H10116 (3)F8—C18—H18106 (4)
O1—C11—C3108.9 (4)F7—C18—H18105 (4)
O1—C11—H11A110 (3)C17—C18—H18120 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C4—H4···O10.88 (5)2.49 (6)2.733 (6)96 (4)
C4—H4···F6i0.88 (5)2.58 (6)3.282 (6)137 (5)
C5—H5···Br20.86 (5)2.68 (5)3.323 (5)133 (4)
C7—H7···F3ii0.91 (6)2.48 (6)3.370 (5)166 (5)
C9—H9···F5iii0.91 (6)2.57 (5)3.466 (5)166 (5)
C9—H9···F2iv0.91 (6)2.58 (6)3.211 (6)127 (4)
C10—H10···F2iv0.97 (6)2.62 (6)3.255 (6)123 (4)
C14—H14···Br1v0.87 (6)2.95 (5)3.744 (4)152 (4)
C14—H14···Br2v0.87 (6)2.96 (5)3.505 (5)122 (4)
C16—H16B···F7vi0.98 (6)2.54 (6)3.208 (6)125 (4)
C16—H16B···F1vii0.98 (6)2.49 (6)3.167 (6)126 (4)
Pt1—Br1···Br1viii2.43 (1)3.69 (1)6.091 (1)168 (1)
C13—F2···F6ix1.35 (1)2.91 (1)4.148 (6)151 (1)
C17—F6···F2x1.37 (1)2.91 (1)3.382 (4)98 (1)
Symmetry codes: (i) x1/2, y+1/2, z1/2; (ii) x+1, y, z+1; (iii) x+1/2, y+1/2, z+3/2; (iv) x+1, y+1, z+1; (v) x+1, y1, z; (vi) x+3/2, y+1/2, z+3/2; (vii) x+1/2, y+1/2, z3/2; (viii) x, y+2, z+1; (ix) x+1/2, y+1/2, z1/2; (x) x+1/2, y+1/2, z+1/2.
 

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