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The [Fe(PM-BiA)2(NCS)2] complex, where PM is N-2-pyridylmethylene and BiA is 4-aminobiphenyl, crystallizes in two polymorphs. The two phases, denoted (I) and (II), undergo a spin-crossover when the sample is cooled and present distinct spin-transition features as (I) shows a very abrupt spin transition, while (II) exhibits a gradual transition. The two forms of the complex are used to investigate the correlations that exist between the spin-transition features and structural features. This article presents the crystal structures of polymorph (II) at room temperature (high spin) and at 120 K (low spin), including a comparison with those of polymorph (I). This study reveals that the packing, in a first approximation, is similar in both forms. In order to look at the crystal structures in more detail, a new angular parameter, denoted θNCS, as well as a particular type of intermolecular hydrogen-bond interaction, which involves the S atoms of the NCS ligands, are investigated. Interestingly, this angle and this intermolecular interaction can be directly connected to the cooperativity of the spin transition. Such a result is extended to all the SCO iron(II) complexes belonging to the same family of the general formula [Fe(PM-L)2(NCS)2].

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108768103011200/na5001sup1.cif
Contains datablocks biamono, bia120K2

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S0108768103011200/na5001biamonosup2.fcf
Contains datablock biamono

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S0108768103011200/na5001bia120K2sup3.fcf
Contains datablock bia120k

CCDC references: 1251853; 1251854

Computing details top

For both compounds, program(s) used to solve structure: SIR 97; program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP 32; software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1]
[Figure 2]
[Figure 3]
[Figure 4]
[Figure 5]
[Figure 6]
[Figure 7]
[Figure 8]
[Figure 9]
[Figure 10]
(biamono) top
Crystal data top
C38H28FeN6S2F(000) = 1424
Mr = 688.63Dx = 1.321 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71069 Å
a = 17.570 (5) ÅCell parameters from 11821 reflections
b = 12.602 (5) Åθ = 1.0–27.5°
c = 17.358 (5) ŵ = 0.59 mm1
β = 115.684 (5)°T = 293 K
V = 3464 (2) Å3Pin, black
Z = 40.15 × 0.1 × 0.1 mm
Data collection top
NONIUS Kappa CCD
diffractometer
3906 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.041
Graphite monochromatorθmax = 25.0°, θmin = 1.3°
Detector resolution: 512 pixels mm-1h = 2020
profile data from ϕ and ω scansk = 1414
23166 measured reflectionsl = 2020
6118 independent reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.052Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.198H atoms treated by a mixture of independent and constrained refinement
S = 1.10 w = 1/[σ2(Fo2) + (0.1242P)2]
where P = (Fo2 + 2Fc2)/3
6118 reflections(Δ/σ)max < 0.001
424 parametersΔρmax = 0.66 e Å3
0 restraintsΔρmin = 0.88 e Å3
Crystal data top
C38H28FeN6S2V = 3464 (2) Å3
Mr = 688.63Z = 4
Monoclinic, P21/cMo Kα radiation
a = 17.570 (5) ŵ = 0.59 mm1
b = 12.602 (5) ÅT = 293 K
c = 17.358 (5) Å0.15 × 0.1 × 0.1 mm
β = 115.684 (5)°
Data collection top
NONIUS Kappa CCD
diffractometer
3906 reflections with I > 2σ(I)
23166 measured reflectionsRint = 0.041
6118 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0520 restraints
wR(F2) = 0.198H atoms treated by a mixture of independent and constrained refinement
S = 1.10Δρmax = 0.66 e Å3
6118 reflectionsΔρmin = 0.88 e Å3
424 parameters
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.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 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 (Å2) top
xyzUiso*/Ueq
Fe10.25924 (3)0.19783 (4)0.32624 (3)0.0664 (2)
S1A0.04611 (8)0.15622 (10)0.42159 (7)0.0918 (4)
S1B0.45240 (8)0.38646 (10)0.57041 (7)0.1002 (4)
N2B0.16745 (19)0.1896 (2)0.18785 (17)0.0668 (8)
N1B0.21054 (19)0.3586 (2)0.29337 (17)0.0666 (7)
N2A0.34728 (19)0.2249 (2)0.26505 (17)0.0665 (7)
N3B0.3483 (2)0.2488 (3)0.44490 (19)0.0823 (9)
N1A0.3108 (2)0.0440 (2)0.32208 (19)0.0830 (10)
N3A0.1732 (3)0.1413 (3)0.3679 (2)0.0976 (11)
C1A0.2944 (4)0.0475 (4)0.3528 (3)0.1137 (17)
H1A0.25650.04730.37710.136*
C2A0.3334 (6)0.1421 (5)0.3488 (4)0.154 (3)
H2A0.32150.20430.37020.184*
C3A0.3899 (7)0.1436 (5)0.3129 (6)0.166 (3)
H3A0.41660.20660.31080.199*
C4A0.4067 (4)0.0518 (4)0.2803 (4)0.133 (2)
H4A0.44420.05120.25560.160*
C5A0.3655 (3)0.0401 (3)0.2858 (3)0.0892 (12)
C6A0.3800 (3)0.1402 (3)0.2526 (2)0.0822 (11)
H6A0.41290.14230.22260.099*
C7A0.3573 (2)0.3221 (3)0.2281 (2)0.0643 (9)
C8A0.3384 (3)0.3274 (3)0.1418 (2)0.0752 (10)
H8A0.32200.26660.10820.090*
C9A0.3440 (3)0.4227 (3)0.1063 (2)0.0830 (11)
H9A0.33230.42540.04870.100*
C10A0.3668 (2)0.5154 (3)0.1546 (2)0.0723 (10)
C11A0.3846 (2)0.5085 (3)0.2411 (2)0.0741 (10)
H11A0.39990.56930.27470.089*
C12A0.3799 (2)0.4125 (3)0.2776 (2)0.0706 (9)
H12A0.39200.40900.33530.085*
C13A0.3754 (3)0.6187 (4)0.1173 (3)0.0920 (13)
C14A0.4255 (4)0.6268 (5)0.0740 (3)0.134 (2)
H14A0.45190.56790.06410.161*
C15A0.4345 (5)0.7324 (9)0.0447 (5)0.186 (5)
H15A0.47120.74150.01960.223*
C16A0.3913 (9)0.8188 (7)0.0527 (7)0.200 (6)
H16A0.39260.88400.02830.240*
C17A0.3506 (8)0.8047 (6)0.0943 (6)0.197 (5)
H17A0.32460.86430.10380.236*
C18A0.3390 (5)0.7106 (5)0.1285 (4)0.141 (2)
H18A0.30670.70930.15910.170*
C19A0.1201 (3)0.1479 (3)0.3906 (2)0.0736 (10)
C1B0.2313 (3)0.4428 (3)0.3460 (2)0.0768 (10)
H1B0.26510.43230.40390.092*
C2B0.2048 (3)0.5427 (3)0.3178 (3)0.0880 (12)
H2B0.22030.59900.35620.106*
C3B0.1556 (3)0.5601 (3)0.2332 (3)0.0979 (13)
H3B0.13740.62830.21310.117*
C4B0.1332 (3)0.4740 (3)0.1773 (3)0.0868 (12)
H4B0.09960.48350.11920.104*
C5B0.1613 (2)0.3752 (3)0.2096 (2)0.0682 (9)
C6B0.1396 (2)0.2805 (3)0.1557 (2)0.0718 (10)
H6B0.10510.28660.09750.086*
C7B0.1483 (2)0.1009 (3)0.1324 (2)0.0649 (9)
C8B0.1534 (3)0.1057 (3)0.0551 (2)0.0748 (10)
H8B0.16920.16860.03800.090*
C9B0.1351 (3)0.0177 (3)0.0036 (2)0.0788 (10)
H9B0.13940.02240.04790.095*
C10B0.1105 (2)0.0781 (3)0.0253 (2)0.0706 (10)
C11B0.1050 (3)0.0813 (3)0.1031 (2)0.0794 (11)
H11B0.08790.14370.11950.095*
C12B0.1244 (3)0.0061 (3)0.1562 (2)0.0775 (10)
H12B0.12140.00130.20830.093*
C13B0.0936 (3)0.1728 (3)0.0308 (2)0.0741 (10)
C14B0.0596 (3)0.1642 (4)0.1190 (2)0.0831 (11)
H14B0.04480.09770.14440.100*
C15B0.0474 (3)0.2530 (4)0.1700 (3)0.0936 (13)
H15B0.02500.24530.22910.112*
C16B0.0679 (3)0.3525 (4)0.1344 (3)0.1029 (15)
H16B0.06030.41170.16890.124*
C17B0.0992 (4)0.3634 (4)0.0487 (3)0.1133 (17)
H17B0.11150.43070.02440.136*
C18B0.1131 (3)0.2750 (3)0.0033 (3)0.0962 (13)
H18B0.13600.28400.06230.115*
C19B0.3918 (3)0.3055 (3)0.4982 (2)0.0728 (10)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Fe10.0845 (4)0.0599 (4)0.0547 (3)0.0033 (2)0.0301 (3)0.0016 (2)
S1A0.0986 (8)0.0980 (8)0.0816 (7)0.0103 (6)0.0417 (6)0.0098 (6)
S1B0.1179 (10)0.0862 (8)0.0926 (8)0.0207 (7)0.0419 (7)0.0232 (6)
N2B0.0726 (19)0.0634 (19)0.0618 (16)0.0051 (15)0.0267 (14)0.0009 (14)
N1B0.0762 (19)0.0655 (19)0.0609 (17)0.0003 (15)0.0325 (14)0.0034 (14)
N2A0.0780 (19)0.0601 (18)0.0592 (16)0.0009 (15)0.0278 (14)0.0033 (13)
N3B0.099 (2)0.086 (2)0.0568 (18)0.0049 (19)0.0287 (16)0.0014 (16)
N1A0.111 (3)0.0570 (19)0.0672 (18)0.0049 (18)0.0253 (17)0.0051 (15)
N3A0.111 (3)0.108 (3)0.083 (2)0.016 (2)0.051 (2)0.008 (2)
C1A0.156 (5)0.076 (3)0.086 (3)0.012 (3)0.032 (3)0.013 (2)
C2A0.233 (9)0.062 (4)0.131 (5)0.002 (4)0.047 (5)0.019 (3)
C3A0.230 (9)0.077 (5)0.172 (7)0.029 (5)0.070 (6)0.000 (4)
C4A0.171 (6)0.075 (4)0.149 (5)0.024 (3)0.065 (4)0.011 (3)
C5A0.108 (3)0.067 (3)0.080 (2)0.010 (2)0.028 (2)0.007 (2)
C6A0.097 (3)0.075 (3)0.081 (3)0.008 (2)0.044 (2)0.006 (2)
C7A0.067 (2)0.066 (2)0.062 (2)0.0035 (17)0.0305 (16)0.0031 (16)
C8A0.097 (3)0.073 (2)0.062 (2)0.014 (2)0.0393 (19)0.0120 (17)
C9A0.097 (3)0.093 (3)0.062 (2)0.019 (2)0.0374 (19)0.003 (2)
C10A0.068 (2)0.074 (2)0.069 (2)0.0145 (19)0.0252 (17)0.0004 (18)
C11A0.079 (2)0.070 (2)0.068 (2)0.0169 (19)0.0261 (18)0.0106 (18)
C12A0.075 (2)0.076 (2)0.0574 (18)0.0049 (19)0.0246 (16)0.0049 (17)
C13A0.090 (3)0.093 (3)0.076 (2)0.034 (3)0.020 (2)0.006 (2)
C14A0.111 (4)0.167 (6)0.116 (4)0.038 (4)0.041 (3)0.032 (4)
C15A0.132 (6)0.252 (10)0.127 (5)0.104 (7)0.011 (4)0.076 (7)
C16A0.253 (13)0.115 (6)0.135 (7)0.079 (7)0.006 (7)0.042 (5)
C17A0.293 (14)0.085 (5)0.137 (7)0.044 (6)0.022 (7)0.030 (4)
C18A0.177 (6)0.090 (4)0.132 (5)0.016 (4)0.043 (4)0.011 (3)
C19A0.092 (3)0.066 (2)0.056 (2)0.018 (2)0.025 (2)0.0024 (16)
C1B0.089 (3)0.068 (2)0.073 (2)0.010 (2)0.035 (2)0.0051 (19)
C2B0.098 (3)0.071 (3)0.093 (3)0.011 (2)0.040 (2)0.014 (2)
C3B0.105 (3)0.066 (3)0.115 (4)0.019 (2)0.041 (3)0.010 (2)
C4B0.096 (3)0.073 (3)0.074 (2)0.010 (2)0.020 (2)0.004 (2)
C5B0.072 (2)0.066 (2)0.066 (2)0.0014 (18)0.0283 (17)0.0026 (17)
C6B0.074 (2)0.075 (3)0.0569 (19)0.0023 (19)0.0190 (16)0.0013 (18)
C7B0.073 (2)0.060 (2)0.0555 (18)0.0056 (17)0.0226 (16)0.0035 (15)
C8B0.094 (3)0.062 (2)0.071 (2)0.0136 (19)0.0383 (19)0.0019 (17)
C9B0.103 (3)0.073 (3)0.067 (2)0.015 (2)0.043 (2)0.0045 (18)
C10B0.075 (2)0.067 (2)0.070 (2)0.0097 (18)0.0314 (18)0.0021 (17)
C11B0.101 (3)0.067 (2)0.074 (2)0.019 (2)0.042 (2)0.0019 (18)
C12B0.100 (3)0.076 (3)0.062 (2)0.015 (2)0.0406 (19)0.0001 (18)
C13B0.082 (3)0.068 (2)0.075 (2)0.0137 (19)0.0366 (19)0.0090 (18)
C14B0.087 (3)0.084 (3)0.077 (3)0.012 (2)0.034 (2)0.003 (2)
C15B0.103 (3)0.100 (3)0.079 (3)0.018 (3)0.041 (2)0.024 (2)
C16B0.123 (4)0.080 (3)0.110 (4)0.019 (3)0.054 (3)0.030 (3)
C17B0.158 (5)0.069 (3)0.113 (4)0.010 (3)0.059 (4)0.014 (3)
C18B0.129 (4)0.075 (3)0.087 (3)0.006 (3)0.049 (3)0.002 (2)
C19B0.092 (3)0.071 (2)0.058 (2)0.004 (2)0.034 (2)0.0063 (18)
Geometric parameters (Å, º) top
Fe1—N3A2.066 (4)C10A—C11A1.398 (5)
Fe1—N3B2.076 (3)C10A—C13A1.490 (6)
Fe1—N1A2.153 (4)C11A—C12A1.384 (5)
Fe1—N1B2.177 (3)C13A—C18A1.377 (8)
Fe1—N2B2.241 (3)C13A—C14A1.387 (7)
Fe1—N2A2.250 (3)C14A—C15A1.457 (10)
S1A—C19A1.612 (5)C15A—C16A1.368 (15)
S1B—C19B1.609 (4)C16A—C17A1.229 (17)
N2B—C6B1.276 (5)C17A—C18A1.380 (9)
N2B—C7B1.417 (4)C1B—C2B1.357 (5)
N1B—C1B1.343 (4)C2B—C3B1.361 (6)
N1B—C5B1.347 (4)C3B—C4B1.395 (6)
N2A—C6A1.275 (5)C4B—C5B1.366 (5)
N2A—C7A1.429 (4)C5B—C6B1.462 (5)
N3B—C19B1.157 (5)C7B—C8B1.384 (5)
N1A—C1A1.354 (6)C7B—C12B1.389 (5)
N1A—C5A1.360 (6)C8B—C9B1.372 (5)
N3A—C19A1.161 (5)C9B—C10B1.389 (5)
C1A—C2A1.392 (9)C10B—C11B1.394 (5)
C2A—C3A1.381 (11)C10B—C13B1.486 (5)
C3A—C4A1.374 (10)C11B—C12B1.380 (5)
C4A—C5A1.390 (7)C13B—C14B1.386 (5)
C5A—C6A1.454 (6)C13B—C18B1.397 (6)
C7A—C12A1.378 (5)C14B—C15B1.385 (6)
C7A—C8A1.388 (5)C15B—C16B1.375 (7)
C8A—C9A1.373 (5)C16B—C17B1.351 (6)
C9A—C10A1.392 (5)C17B—C18B1.387 (6)
N3A—Fe1—N3B96.35 (14)C9A—C10A—C11A117.8 (3)
N3A—Fe1—N1A94.78 (16)C9A—C10A—C13A121.9 (3)
N3B—Fe1—N1A99.47 (13)C11A—C10A—C13A120.3 (3)
N3A—Fe1—N1B98.55 (15)C12A—C11A—C10A121.1 (3)
N3B—Fe1—N1B90.79 (13)C7A—C12A—C11A119.7 (3)
N1A—Fe1—N1B162.17 (12)C18A—C13A—C14A117.2 (5)
N3A—Fe1—N2B93.64 (13)C18A—C13A—C10A122.2 (5)
N3B—Fe1—N2B163.85 (12)C14A—C13A—C10A120.5 (5)
N1A—Fe1—N2B92.29 (11)C13A—C14A—C15A116.5 (7)
N1B—Fe1—N2B75.16 (10)C16A—C15A—C14A122.8 (9)
N3A—Fe1—N2A167.21 (13)C17A—C16A—C15A115.7 (9)
N3B—Fe1—N2A92.57 (12)C16A—C17A—C18A127.4 (12)
N1A—Fe1—N2A74.66 (13)C13A—C18A—C17A119.9 (8)
N1B—Fe1—N2A90.45 (11)N3A—C19A—S1A179.5 (4)
N2B—Fe1—N2A79.84 (11)N1B—C1B—C2B122.6 (3)
C6B—N2B—C7B118.6 (3)C1B—C2B—C3B119.8 (4)
C6B—N2B—Fe1112.8 (2)C2B—C3B—C4B118.7 (4)
C7B—N2B—Fe1127.8 (2)C5B—C4B—C3B118.7 (4)
C1B—N1B—C5B118.0 (3)N1B—C5B—C4B122.2 (3)
C1B—N1B—Fe1126.7 (2)N1B—C5B—C6B115.6 (3)
C5B—N1B—Fe1115.0 (2)C4B—C5B—C6B122.2 (3)
C6A—N2A—C7A119.3 (3)N2B—C6B—C5B120.6 (3)
C6A—N2A—Fe1114.0 (3)C8B—C7B—C12B118.8 (3)
C7A—N2A—Fe1125.8 (2)C8B—C7B—N2B121.9 (3)
C19B—N3B—Fe1159.6 (3)C12B—C7B—N2B119.3 (3)
C1A—N1A—C5A117.7 (4)C9B—C8B—C7B120.1 (3)
C1A—N1A—Fe1126.2 (4)C8B—C9B—C10B122.5 (3)
C5A—N1A—Fe1116.1 (3)C9B—C10B—C11B116.6 (3)
C19A—N3A—Fe1155.6 (4)C9B—C10B—C13B121.1 (3)
N1A—C1A—C2A121.1 (6)C11B—C10B—C13B122.2 (3)
C3A—C2A—C1A120.0 (6)C12B—C11B—C10B121.6 (3)
C4A—C3A—C2A119.9 (7)C11B—C12B—C7B120.4 (3)
C3A—C4A—C5A117.5 (7)C14B—C13B—C18B116.7 (4)
N1A—C5A—C4A123.8 (5)C14B—C13B—C10B122.0 (4)
N1A—C5A—C6A115.6 (4)C18B—C13B—C10B121.3 (4)
C4A—C5A—C6A120.6 (5)C15B—C14B—C13B121.1 (4)
N2A—C6A—C5A119.3 (4)C16B—C15B—C14B120.8 (4)
C12A—C7A—C8A120.2 (3)C17B—C16B—C15B119.4 (4)
C12A—C7A—N2A119.2 (3)C16B—C17B—C18B120.5 (5)
C8A—C7A—N2A120.4 (3)C17B—C18B—C13B121.5 (4)
C9A—C8A—C7A119.7 (3)N3B—C19B—S1B178.5 (4)
C8A—C9A—C10A121.5 (3)
(bia120K2) top
Crystal data top
C38H28FeN6S2F(000) = 1424
Mr = 688.63Dx = 1.389 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71069 Å
a = 17.362 (5) ÅCell parameters from 14905 reflections
b = 12.362 (5) Åθ = 1.0–27.5°
c = 17.050 (5) ŵ = 0.62 mm1
β = 115.833 (5)°T = 120 K
V = 3293.7 (19) Å3Pin, black
Z = 40.15 × 0.1 × 0.1 mm
Data collection top
BRUCKER-NONIUS Kappa CCD
diffractometer
5536 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.053
Graphite monochromatorθmax = 27.5°, θmin = 1.3°
Detector resolution: 512 pixels mm-1h = 2222
profile data from ϕ and ω scansk = 1616
29088 measured reflectionsl = 2222
7540 independent reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.039Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.144H atoms treated by a mixture of independent and constrained refinement
S = 1.20 w = 1/[σ2(Fo2) + (0.078P)2 + 0.0869P]
where P = (Fo2 + 2Fc2)/3
7540 reflections(Δ/σ)max = 0.001
424 parametersΔρmax = 0.68 e Å3
0 restraintsΔρmin = 1.00 e Å3
Crystal data top
C38H28FeN6S2V = 3293.7 (19) Å3
Mr = 688.63Z = 4
Monoclinic, P21/cMo Kα radiation
a = 17.362 (5) ŵ = 0.62 mm1
b = 12.362 (5) ÅT = 120 K
c = 17.050 (5) Å0.15 × 0.1 × 0.1 mm
β = 115.833 (5)°
Data collection top
BRUCKER-NONIUS Kappa CCD
diffractometer
5536 reflections with I > 2σ(I)
29088 measured reflectionsRint = 0.053
7540 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0390 restraints
wR(F2) = 0.144H atoms treated by a mixture of independent and constrained refinement
S = 1.20Δρmax = 0.68 e Å3
7540 reflectionsΔρmin = 1.00 e Å3
424 parameters
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.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 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 (Å2) top
xyzUiso*/Ueq
Fe10.25556 (2)0.20960 (3)0.31322 (2)0.02212 (12)
S1A0.04588 (4)0.16746 (5)0.41723 (4)0.02846 (17)
S1B0.44775 (4)0.36214 (6)0.57792 (4)0.03246 (18)
N2B0.16998 (13)0.19720 (15)0.19095 (12)0.0233 (4)
N1B0.21424 (13)0.36016 (16)0.29432 (12)0.0225 (4)
N2A0.34026 (13)0.23379 (16)0.26745 (12)0.0240 (5)
N3B0.33999 (13)0.24355 (17)0.43120 (13)0.0260 (5)
N1A0.29952 (13)0.06185 (16)0.32269 (12)0.0275 (5)
N3A0.17182 (14)0.17349 (17)0.35653 (13)0.0275 (5)
C1A0.27644 (18)0.0255 (2)0.35434 (16)0.0350 (6)
H1A0.23360.01820.37440.042*
C2A0.3136 (2)0.1262 (2)0.35847 (19)0.0479 (8)
H2A0.29490.18710.37950.058*
C3A0.3776 (2)0.1376 (2)0.3320 (2)0.0530 (9)
H3A0.40460.20560.33620.064*
C4A0.4019 (2)0.0484 (2)0.29915 (19)0.0457 (8)
H4A0.44530.05430.27960.055*
C5A0.36176 (17)0.0495 (2)0.29533 (16)0.0317 (6)
C6A0.38092 (17)0.1488 (2)0.26218 (16)0.0311 (6)
H6A0.42100.15120.23800.037*
C7A0.35227 (16)0.3334 (2)0.23110 (15)0.0246 (5)
C8A0.33329 (17)0.3389 (2)0.14318 (16)0.0286 (6)
H8A0.31560.27590.10780.034*
C9A0.34045 (17)0.4374 (2)0.10729 (17)0.0305 (6)
H9A0.32830.44100.04740.037*
C10A0.36536 (16)0.5310 (2)0.15835 (16)0.0278 (6)
C11A0.38390 (16)0.5230 (2)0.24634 (16)0.0292 (6)
H11A0.40070.58600.28170.035*
C12A0.37839 (16)0.4252 (2)0.28336 (15)0.0268 (6)
H12A0.39230.42090.34370.032*
C13A0.37406 (17)0.6366 (2)0.12117 (16)0.0321 (6)
C14A0.4215 (2)0.6451 (3)0.07349 (18)0.0434 (8)
H14A0.44630.58240.06180.052*
C15A0.4327 (2)0.7462 (3)0.0427 (2)0.0568 (10)
H15A0.46640.75170.01150.068*
C16A0.3956 (2)0.8369 (3)0.0569 (2)0.0591 (10)
H16A0.40330.90490.03540.071*
C17A0.3477 (2)0.8295 (3)0.1020 (2)0.0594 (10)
H17A0.32090.89240.11070.071*
C18A0.3375 (2)0.7306 (2)0.13553 (19)0.0434 (7)
H18A0.30540.72710.16850.052*
C19A0.11958 (17)0.17121 (19)0.38190 (15)0.0244 (5)
C1B0.23620 (16)0.4428 (2)0.35150 (15)0.0264 (5)
H1B0.27250.42850.41110.032*
C2B0.20819 (16)0.5470 (2)0.32719 (16)0.0290 (6)
H2B0.22610.60330.36940.035*
C3B0.15396 (17)0.5697 (2)0.24129 (16)0.0315 (6)
H3B0.13460.64140.22350.038*
C4B0.12833 (17)0.4854 (2)0.18162 (16)0.0286 (6)
H4B0.09020.49810.12230.034*
C5B0.15911 (16)0.38275 (19)0.20980 (15)0.0243 (5)
C6B0.13582 (16)0.28799 (19)0.15430 (15)0.0239 (5)
H6B0.09750.29220.09420.029*
C7B0.15008 (15)0.10239 (19)0.13616 (14)0.0232 (5)
C8B0.15848 (16)0.1047 (2)0.05907 (15)0.0268 (6)
H8B0.17740.16880.04200.032*
C9B0.13913 (16)0.0132 (2)0.00685 (16)0.0273 (6)
H9B0.14470.01550.04610.033*
C10B0.11173 (15)0.08201 (19)0.03035 (15)0.0241 (5)
C11B0.10235 (16)0.0821 (2)0.10783 (15)0.0274 (6)
H11B0.08220.14540.12450.033*
C12B0.12209 (16)0.00905 (19)0.16076 (15)0.0253 (5)
H12B0.11640.00740.21370.030*
C13B0.09505 (16)0.1808 (2)0.02487 (15)0.0250 (5)
C14B0.06206 (16)0.1733 (2)0.11543 (16)0.0277 (6)
H14B0.04770.10430.14260.033*
C15B0.04987 (17)0.2653 (2)0.16665 (17)0.0308 (6)
H15B0.02700.25890.22820.037*
C16B0.07110 (17)0.3661 (2)0.12785 (17)0.0325 (6)
H16B0.06380.42890.16250.039*
C17B0.10299 (18)0.3749 (2)0.03830 (17)0.0328 (6)
H17B0.11670.44410.01150.039*
C18B0.11512 (17)0.2834 (2)0.01255 (17)0.0295 (6)
H18B0.13750.29060.07400.035*
C19B0.38556 (16)0.2902 (2)0.49329 (16)0.0247 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Fe10.0271 (2)0.0163 (2)0.0200 (2)0.00060 (14)0.00748 (15)0.00079 (13)
S1A0.0328 (4)0.0263 (4)0.0260 (3)0.0036 (3)0.0125 (3)0.0013 (3)
S1B0.0341 (4)0.0316 (4)0.0285 (4)0.0042 (3)0.0108 (3)0.0090 (3)
N2B0.0274 (11)0.0192 (11)0.0217 (10)0.0009 (9)0.0091 (9)0.0010 (8)
N1B0.0264 (11)0.0188 (11)0.0214 (10)0.0002 (8)0.0097 (9)0.0005 (8)
N2A0.0274 (11)0.0210 (11)0.0198 (10)0.0005 (9)0.0069 (9)0.0004 (8)
N3B0.0298 (12)0.0219 (11)0.0230 (11)0.0018 (9)0.0084 (9)0.0035 (9)
N1A0.0311 (12)0.0202 (11)0.0231 (10)0.0015 (9)0.0042 (9)0.0014 (8)
N3A0.0316 (12)0.0252 (11)0.0227 (11)0.0011 (9)0.0091 (10)0.0022 (9)
C1A0.0407 (16)0.0225 (14)0.0289 (14)0.0023 (12)0.0032 (12)0.0047 (11)
C2A0.057 (2)0.0222 (15)0.0453 (18)0.0004 (14)0.0048 (16)0.0054 (13)
C3A0.070 (2)0.0227 (16)0.053 (2)0.0161 (15)0.0143 (18)0.0025 (14)
C4A0.056 (2)0.0313 (17)0.0475 (17)0.0159 (15)0.0197 (15)0.0002 (14)
C5A0.0382 (16)0.0235 (14)0.0277 (13)0.0074 (12)0.0091 (12)0.0014 (11)
C6A0.0323 (15)0.0320 (15)0.0284 (14)0.0060 (12)0.0127 (12)0.0010 (11)
C7A0.0230 (13)0.0252 (13)0.0259 (13)0.0010 (10)0.0109 (10)0.0013 (10)
C8A0.0325 (15)0.0261 (14)0.0273 (14)0.0015 (11)0.0132 (11)0.0042 (11)
C9A0.0332 (15)0.0331 (15)0.0271 (13)0.0002 (12)0.0148 (11)0.0022 (11)
C10A0.0236 (13)0.0279 (14)0.0307 (13)0.0026 (11)0.0106 (11)0.0007 (11)
C11A0.0245 (13)0.0288 (14)0.0309 (14)0.0048 (11)0.0090 (11)0.0060 (11)
C12A0.0270 (13)0.0290 (14)0.0215 (12)0.0010 (11)0.0080 (10)0.0005 (10)
C13A0.0265 (14)0.0333 (15)0.0289 (14)0.0087 (11)0.0049 (11)0.0023 (11)
C14A0.0399 (18)0.050 (2)0.0386 (16)0.0114 (14)0.0153 (14)0.0061 (14)
C15A0.047 (2)0.075 (3)0.0393 (18)0.0293 (19)0.0102 (15)0.0118 (17)
C16A0.066 (2)0.044 (2)0.0408 (19)0.0267 (18)0.0020 (17)0.0111 (16)
C17A0.071 (3)0.0319 (18)0.052 (2)0.0044 (17)0.0050 (18)0.0047 (16)
C18A0.0449 (18)0.0333 (17)0.0440 (17)0.0015 (14)0.0119 (14)0.0043 (13)
C19A0.0315 (14)0.0154 (12)0.0183 (12)0.0017 (10)0.0033 (11)0.0012 (9)
C1B0.0309 (14)0.0238 (13)0.0230 (12)0.0016 (11)0.0105 (10)0.0031 (10)
C2B0.0323 (15)0.0209 (13)0.0318 (14)0.0005 (11)0.0122 (11)0.0051 (11)
C3B0.0399 (16)0.0184 (13)0.0357 (15)0.0044 (11)0.0158 (12)0.0021 (11)
C4B0.0335 (15)0.0233 (14)0.0245 (13)0.0042 (11)0.0085 (11)0.0020 (10)
C5B0.0269 (13)0.0210 (13)0.0238 (12)0.0000 (10)0.0100 (10)0.0003 (10)
C6B0.0263 (13)0.0218 (13)0.0210 (12)0.0011 (10)0.0079 (10)0.0017 (10)
C7B0.0254 (13)0.0186 (12)0.0212 (12)0.0009 (10)0.0060 (10)0.0030 (9)
C8B0.0331 (14)0.0174 (13)0.0277 (13)0.0037 (10)0.0111 (11)0.0020 (10)
C9B0.0362 (15)0.0214 (13)0.0258 (13)0.0001 (11)0.0149 (11)0.0005 (10)
C10B0.0249 (13)0.0193 (13)0.0256 (12)0.0008 (10)0.0086 (10)0.0019 (10)
C11B0.0317 (14)0.0212 (13)0.0287 (13)0.0029 (11)0.0127 (11)0.0000 (10)
C12B0.0301 (14)0.0227 (13)0.0212 (12)0.0007 (10)0.0094 (11)0.0000 (10)
C13B0.0250 (13)0.0210 (13)0.0297 (13)0.0029 (10)0.0125 (11)0.0023 (10)
C14B0.0294 (14)0.0230 (13)0.0288 (14)0.0026 (11)0.0108 (11)0.0003 (11)
C15B0.0328 (15)0.0308 (15)0.0276 (14)0.0052 (12)0.0120 (11)0.0056 (11)
C16B0.0357 (16)0.0280 (15)0.0370 (15)0.0052 (12)0.0188 (13)0.0099 (11)
C17B0.0419 (16)0.0200 (13)0.0368 (15)0.0016 (12)0.0173 (13)0.0009 (11)
C18B0.0372 (15)0.0253 (14)0.0258 (13)0.0014 (11)0.0137 (12)0.0011 (10)
C19B0.0265 (14)0.0231 (13)0.0251 (13)0.0040 (11)0.0119 (11)0.0052 (10)
Geometric parameters (Å, º) top
Fe1—N3A1.948 (2)C10A—C11A1.394 (4)
Fe1—N3B1.950 (2)C10A—C13A1.487 (4)
Fe1—N1A1.959 (2)C11A—C12A1.386 (4)
Fe1—N2A1.965 (2)C13A—C14A1.391 (4)
Fe1—N2B1.969 (2)C13A—C18A1.396 (4)
Fe1—N1B1.970 (2)C14A—C15A1.401 (4)
S1A—C19A1.635 (3)C15A—C16A1.366 (5)
S1B—C19B1.638 (3)C16A—C17A1.360 (5)
N2B—C6B1.296 (3)C17A—C18A1.393 (4)
N2B—C7B1.444 (3)C1B—C2B1.375 (3)
N1B—C1B1.348 (3)C2B—C3B1.381 (4)
N1B—C5B1.367 (3)C3B—C4B1.387 (4)
N2A—C6A1.291 (3)C4B—C5B1.379 (3)
N2A—C7A1.434 (3)C5B—C6B1.448 (3)
N3B—C19B1.161 (3)C7B—C8B1.384 (3)
N1A—C1A1.344 (3)C7B—C12B1.386 (3)
N1A—C5A1.359 (3)C8B—C9B1.388 (3)
N3A—C19A1.163 (3)C9B—C10B1.392 (3)
C1A—C2A1.390 (4)C10B—C11B1.400 (3)
C2A—C3A1.376 (5)C10B—C13B1.491 (3)
C3A—C4A1.383 (4)C11B—C12B1.390 (3)
C4A—C5A1.383 (4)C13B—C18B1.394 (3)
C5A—C6A1.450 (4)C13B—C14B1.396 (3)
C7A—C8A1.389 (3)C14B—C15B1.393 (4)
C7A—C12A1.391 (3)C15B—C16B1.383 (4)
C8A—C9A1.392 (4)C16B—C17B1.383 (4)
C9A—C10A1.399 (4)C17B—C18B1.385 (3)
N3A—Fe1—N3B90.46 (9)C11A—C10A—C9A118.3 (2)
N3A—Fe1—N1A94.79 (9)C11A—C10A—C13A120.2 (2)
N3B—Fe1—N1A91.42 (9)C9A—C10A—C13A121.5 (2)
N3A—Fe1—N2A175.45 (9)C12A—C11A—C10A121.5 (2)
N3B—Fe1—N2A91.18 (9)C11A—C12A—C7A119.2 (2)
N1A—Fe1—N2A80.94 (9)C14A—C13A—C18A118.0 (3)
N3A—Fe1—N2B92.29 (9)C14A—C13A—C10A120.8 (3)
N3B—Fe1—N2B171.98 (8)C18A—C13A—C10A121.2 (3)
N1A—Fe1—N2B95.85 (8)C13A—C14A—C15A120.1 (3)
N2A—Fe1—N2B86.64 (8)C16A—C15A—C14A120.8 (3)
N3A—Fe1—N1B89.99 (9)C17A—C16A—C15A119.8 (3)
N3B—Fe1—N1B91.25 (8)C16A—C17A—C18A120.6 (4)
N1A—Fe1—N1B174.51 (8)C17A—C18A—C13A120.7 (3)
N2A—Fe1—N1B94.22 (8)N3A—C19A—S1A179.7 (3)
N2B—Fe1—N1B81.22 (8)N1B—C1B—C2B122.7 (2)
C6B—N2B—C7B117.45 (19)C1B—C2B—C3B119.8 (2)
C6B—N2B—Fe1114.75 (16)C2B—C3B—C4B118.6 (2)
C7B—N2B—Fe1127.27 (15)C5B—C4B—C3B118.9 (2)
C1B—N1B—C5B117.1 (2)N1B—C5B—C4B122.8 (2)
C1B—N1B—Fe1129.06 (16)N1B—C5B—C6B113.0 (2)
C5B—N1B—Fe1113.78 (15)C4B—C5B—C6B124.1 (2)
C6A—N2A—C7A118.8 (2)N2B—C6B—C5B116.5 (2)
C6A—N2A—Fe1115.50 (18)C8B—C7B—C12B120.0 (2)
C7A—N2A—Fe1125.25 (16)C8B—C7B—N2B120.2 (2)
C19B—N3B—Fe1162.7 (2)C12B—C7B—N2B119.8 (2)
C1A—N1A—C5A117.9 (2)C7B—C8B—C9B119.7 (2)
C1A—N1A—Fe1127.5 (2)C8B—C9B—C10B121.5 (2)
C5A—N1A—Fe1114.59 (17)C9B—C10B—C11B117.9 (2)
C19A—N3A—Fe1168.1 (2)C9B—C10B—C13B120.5 (2)
N1A—C1A—C2A121.8 (3)C11B—C10B—C13B121.6 (2)
C3A—C2A—C1A119.9 (3)C12B—C11B—C10B121.0 (2)
C2A—C3A—C4A118.9 (3)C7B—C12B—C11B119.9 (2)
C3A—C4A—C5A118.7 (3)C18B—C13B—C14B117.8 (2)
N1A—C5A—C4A122.8 (3)C18B—C13B—C10B121.0 (2)
N1A—C5A—C6A113.0 (2)C14B—C13B—C10B121.1 (2)
C4A—C5A—C6A124.2 (3)C15B—C14B—C13B121.1 (2)
N2A—C6A—C5A115.9 (2)C16B—C15B—C14B120.0 (2)
C8A—C7A—C12A120.6 (2)C17B—C16B—C15B119.6 (2)
C8A—C7A—N2A119.8 (2)C16B—C17B—C18B120.4 (2)
C12A—C7A—N2A119.5 (2)C17B—C18B—C13B121.2 (2)
C7A—C8A—C9A119.5 (2)N3B—C19B—S1B176.8 (2)
C8A—C9A—C10A120.8 (2)

Experimental details

(biamono)(bia120K2)
Crystal data
Chemical formulaC38H28FeN6S2C38H28FeN6S2
Mr688.63688.63
Crystal system, space groupMonoclinic, P21/cMonoclinic, P21/c
Temperature (K)293120
a, b, c (Å)17.570 (5), 12.602 (5), 17.358 (5)17.362 (5), 12.362 (5), 17.050 (5)
β (°) 115.684 (5) 115.833 (5)
V3)3464 (2)3293.7 (19)
Z44
Radiation typeMo KαMo Kα
µ (mm1)0.590.62
Crystal size (mm)0.15 × 0.1 × 0.10.15 × 0.1 × 0.1
Data collection
DiffractometerNONIUS Kappa CCD
diffractometer
BRUCKER-NONIUS Kappa CCD
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
23166, 6118, 3906 29088, 7540, 5536
Rint0.0410.053
(sin θ/λ)max1)0.5950.649
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.052, 0.198, 1.10 0.039, 0.144, 1.20
No. of reflections61187540
No. of parameters424424
H-atom treatmentH atoms treated by a mixture of independent and constrained refinementH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.66, 0.880.68, 1.00

Computer programs: SIR 97, SHELXL97 (Sheldrick, 1997), ORTEP 32, SHELXL97.

 

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