Literature DB >> 22412402

Bis[(2-chloro-4-fluoro-benz-yl)triphenyl-phospho-nium] bis-(1,2,5-thia-diazole-3,4-dithiol-ato)nickelate(II).

Zhou-Hua Zeng1, Shui-Bin Yang.   

Abstract

The title ion-pair complex, (C(25)H(20)ClFP)(2)[Ni(C(2)N(2)S(3))(2)], was obtained by the direct reaction of (4-F,2-ClBzTPP)(+)·Br(-) [4-F,2-ClBzTPP(+) is (2-chloro-4-fluoro-benz-yl)triphenyl-phos-pho-nium], NiCl(2)·6H(2)O and Na(2)tdas (tdas(2-) is 1,2,5-thia-diazole-3,4-dithiol-ate) in methanol. The asymmetric unit of the title structure comprises one (4-F,2-ClBzTPP)(+) cation and half of an [Ni(tdas)(2)](2-) complex anion, with the Ni(II) ion situated on a center of symmetry, leading to a slightly distorted square-planar coordination of the latter. In the cation, the tetra-hedral angles around the P atom are nearly undistorted. In the crystal, the cations and anions are linked by C-H⋯S, C-H⋯N and C-H⋯Cl hydrogen bonds.

Entities:  

Year:  2012        PMID: 22412402      PMCID: PMC3297212          DOI: 10.1107/S1600536812003625

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For background to complexes containing the [Ni(maleo­nitrile­dithiol­ate)2]2− anion, see: Chen et al. (2010 ▶); Hou et al. (2008 ▶); Ni et al. (2005 ▶); Ren et al. (2002 ▶); Robertson & Cronin (2002 ▶); Xie et al. (2002 ▶); Zhou et al. (2011 ▶). For details of other square-planar Ni(1,2,5-thia­diazole-3,4-dithiol­ate)2 complexes, see: Awaga et al. (1994 ▶); Yamochi et al. (2001 ▶); Okuno et al. (2003 ▶); Ni et al. (2004 ▶); Zuo et al. (2009 ▶).

Experimental

Crystal data

(C25H20ClFP)2[Ni(C2N2S3)2] M = 1166.81 Triclinic, a = 9.4447 (11) Å b = 12.1385 (15) Å c = 13.1309 (16) Å α = 71.447 (1)° β = 83.601 (2)° γ = 68.691 (2)° V = 1329.6 (3) Å3 Z = 1 Mo Kα radiation μ = 0.81 mm−1 T = 291 K 0.19 × 0.15 × 0.11 mm

Data collection

Bruker SMART CCD diffractometer Absorption correction: multi-scan (SADABS; Bruker, 2004 ▶) T min = 0.861, T max = 0.916 9694 measured reflections 4652 independent reflections 3807 reflections with I > 2σ(I) R int = 0.033

Refinement

R[F 2 > 2σ(F 2)] = 0.042 wR(F 2) = 0.118 S = 1.00 4652 reflections 322 parameters H-atom parameters constrained Δρmax = 0.54 e Å−3 Δρmin = −0.39 e Å−3 Data collection: SMART (Bruker, 2004 ▶); cell refinement: SAINT (Bruker, 2004 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL. Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812003625/wm2587sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812003625/wm2587Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
(C25H20ClFP)2[Ni(C2N2S3)2]Z = 1
Mr = 1166.81F(000) = 598
Triclinic, P1Dx = 1.457 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 9.4447 (11) ÅCell parameters from 3884 reflections
b = 12.1385 (15) Åθ = 2.3–26.0°
c = 13.1309 (16) ŵ = 0.81 mm1
α = 71.447 (1)°T = 291 K
β = 83.601 (2)°Block, brown
γ = 68.691 (2)°0.19 × 0.15 × 0.11 mm
V = 1329.6 (3) Å3
Bruker SMART CCD diffractometer4652 independent reflections
Radiation source: fine-focus sealed tube3807 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.033
φ and ω scansθmax = 25.0°, θmin = 1.6°
Absorption correction: multi-scan (SADABS; Bruker, 2004)h = −11→10
Tmin = 0.861, Tmax = 0.916k = −14→14
9694 measured reflectionsl = −15→15
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.042Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.118H-atom parameters constrained
S = 1.00w = 1/[σ2(Fo2) + (0.0368P)2 + 1.988P] where P = (Fo2 + 2Fc2)/3
4652 reflections(Δ/σ)max < 0.001
322 parametersΔρmax = 0.54 e Å3
0 restraintsΔρmin = −0.39 e Å3
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.
xyzUiso*/Ueq
Ni10.50000.50000.00000.03811 (17)
S10.58693 (12)0.34739 (9)−0.07028 (7)0.0552 (3)
S20.42586 (13)0.38755 (9)0.14777 (8)0.0618 (3)
S30.49400 (15)0.04337 (10)0.12386 (9)0.0728 (3)
Cl10.70371 (13)0.46088 (10)0.42942 (8)0.0685 (3)
F10.5385 (4)0.1177 (3)0.4145 (3)0.1061 (10)
N10.5634 (4)0.1203 (3)0.0147 (3)0.0644 (9)
N20.4341 (4)0.1508 (3)0.1854 (3)0.0654 (9)
P10.95727 (10)0.22890 (8)0.69433 (7)0.0408 (2)
C10.5392 (4)0.2291 (3)0.0242 (3)0.0459 (8)
C20.4655 (4)0.2480 (3)0.1213 (3)0.0475 (8)
C30.6640 (4)0.3250 (3)0.4940 (3)0.0505 (8)
C40.6126 (5)0.2753 (4)0.4295 (3)0.0632 (11)
H40.59920.31360.35590.076*
C50.5826 (5)0.1690 (4)0.4779 (4)0.0684 (11)
C60.5948 (5)0.1121 (4)0.5864 (4)0.0680 (11)
H60.56860.04180.61720.082*
C70.6469 (4)0.1618 (4)0.6486 (3)0.0544 (9)
H70.65650.12360.72240.065*
C80.6859 (4)0.2682 (3)0.6042 (3)0.0436 (8)
C90.7547 (4)0.3131 (3)0.6737 (3)0.0456 (8)
H9A0.70420.30380.74290.055*
H9B0.73760.40060.64040.055*
C100.8961 (5)0.0449 (4)0.8608 (3)0.0588 (10)
H100.81380.10870.87530.071*
C110.9250 (6)−0.0750 (4)0.9244 (3)0.0738 (12)
H110.8615−0.09250.98190.089*
C121.0475 (6)−0.1698 (5)0.9035 (4)0.0797 (14)
H121.0651−0.25110.94610.096*
C131.1436 (5)−0.1448 (4)0.8202 (4)0.0717 (12)
H131.2272−0.20890.80750.086*
C141.1167 (4)−0.0246 (3)0.7551 (3)0.0553 (9)
H141.1824−0.00760.69900.066*
C150.9911 (4)0.0703 (3)0.7741 (3)0.0454 (8)
C160.9476 (5)0.3957 (4)0.8019 (3)0.0583 (10)
H160.84260.42580.79330.070*
C171.0149 (6)0.4456 (5)0.8554 (4)0.0757 (13)
H170.95530.50920.88320.091*
C181.1704 (6)0.4007 (5)0.8674 (4)0.0777 (13)
H181.21520.43470.90320.093*
C191.2600 (5)0.3067 (5)0.8274 (4)0.0760 (13)
H191.36500.27770.83520.091*
C201.1938 (5)0.2558 (4)0.7757 (3)0.0673 (11)
H201.25400.19040.75010.081*
C211.0368 (4)0.3015 (3)0.7614 (3)0.0475 (8)
C221.1227 (4)0.3129 (3)0.5183 (3)0.0559 (9)
H221.13550.36250.55530.067*
C231.1813 (5)0.3194 (4)0.4163 (4)0.0721 (12)
H231.23530.37240.38550.087*
C241.1614 (5)0.2499 (5)0.3607 (4)0.0773 (14)
H241.20110.25590.29190.093*
C251.0820 (5)0.1692 (4)0.4052 (3)0.0663 (11)
H251.06780.12210.36620.080*
C261.0242 (4)0.1596 (3)0.5083 (3)0.0524 (9)
H260.97210.10520.53940.063*
C271.0450 (4)0.2327 (3)0.5651 (3)0.0439 (8)
U11U22U33U12U13U23
Ni10.0364 (3)0.0470 (4)0.0314 (3)−0.0127 (3)0.0052 (2)−0.0163 (2)
S10.0713 (6)0.0579 (6)0.0441 (5)−0.0277 (5)0.0236 (4)−0.0269 (4)
S20.0861 (7)0.0503 (5)0.0480 (5)−0.0237 (5)0.0288 (5)−0.0230 (4)
S30.0978 (9)0.0573 (6)0.0710 (7)−0.0355 (6)0.0188 (6)−0.0257 (5)
Cl10.0798 (7)0.0599 (6)0.0587 (6)−0.0315 (5)−0.0064 (5)0.0020 (5)
F10.123 (3)0.127 (3)0.108 (2)−0.064 (2)−0.0197 (19)−0.056 (2)
N10.085 (2)0.055 (2)0.061 (2)−0.0268 (18)0.0149 (17)−0.0296 (16)
N20.082 (2)0.057 (2)0.059 (2)−0.0284 (18)0.0207 (17)−0.0200 (16)
P10.0422 (5)0.0435 (5)0.0385 (4)−0.0172 (4)0.0047 (4)−0.0137 (4)
C10.0465 (19)0.048 (2)0.0452 (19)−0.0146 (16)0.0030 (15)−0.0204 (16)
C20.0447 (19)0.054 (2)0.0430 (18)−0.0168 (16)0.0083 (15)−0.0157 (16)
C30.046 (2)0.054 (2)0.050 (2)−0.0155 (17)0.0012 (16)−0.0157 (17)
C40.058 (2)0.079 (3)0.052 (2)−0.019 (2)−0.0064 (18)−0.022 (2)
C50.063 (3)0.081 (3)0.077 (3)−0.029 (2)−0.010 (2)−0.036 (3)
C60.066 (3)0.067 (3)0.083 (3)−0.037 (2)−0.003 (2)−0.021 (2)
C70.050 (2)0.061 (2)0.054 (2)−0.0263 (18)0.0026 (17)−0.0123 (18)
C80.0367 (17)0.0486 (19)0.0444 (18)−0.0121 (15)0.0041 (14)−0.0168 (15)
C90.0443 (19)0.050 (2)0.0436 (18)−0.0154 (16)0.0045 (15)−0.0182 (16)
C100.059 (2)0.069 (3)0.044 (2)−0.024 (2)0.0023 (17)−0.0088 (18)
C110.083 (3)0.078 (3)0.052 (2)−0.040 (3)−0.002 (2)0.006 (2)
C120.098 (4)0.063 (3)0.068 (3)−0.037 (3)−0.025 (3)0.011 (2)
C130.075 (3)0.056 (3)0.073 (3)−0.013 (2)−0.019 (2)−0.010 (2)
C140.053 (2)0.054 (2)0.056 (2)−0.0165 (18)−0.0012 (17)−0.0143 (18)
C150.0471 (19)0.052 (2)0.0387 (17)−0.0216 (16)−0.0003 (15)−0.0098 (15)
C160.059 (2)0.064 (2)0.060 (2)−0.022 (2)0.0012 (18)−0.029 (2)
C170.083 (3)0.083 (3)0.077 (3)−0.032 (3)−0.001 (2)−0.041 (3)
C180.094 (4)0.091 (3)0.068 (3)−0.050 (3)−0.013 (3)−0.025 (3)
C190.066 (3)0.088 (3)0.081 (3)−0.029 (3)−0.018 (2)−0.027 (3)
C200.054 (2)0.074 (3)0.074 (3)−0.015 (2)−0.012 (2)−0.027 (2)
C210.052 (2)0.052 (2)0.0408 (18)−0.0230 (17)−0.0022 (15)−0.0108 (15)
C220.060 (2)0.051 (2)0.058 (2)−0.0253 (19)0.0099 (18)−0.0135 (18)
C230.072 (3)0.073 (3)0.068 (3)−0.038 (2)0.025 (2)−0.011 (2)
C240.075 (3)0.085 (3)0.055 (2)−0.020 (3)0.029 (2)−0.016 (2)
C250.071 (3)0.072 (3)0.053 (2)−0.016 (2)0.013 (2)−0.030 (2)
C260.054 (2)0.057 (2)0.048 (2)−0.0209 (18)0.0103 (16)−0.0185 (17)
C270.0429 (18)0.0435 (19)0.0437 (18)−0.0155 (15)0.0081 (14)−0.0132 (15)
Ni1—S1i2.1842 (9)C10—H100.9300
Ni1—S12.1842 (9)C11—C121.379 (7)
Ni1—S2i2.1966 (9)C11—H110.9300
Ni1—S22.1966 (9)C12—C131.371 (7)
S1—C11.736 (4)C12—H120.9300
S2—C21.737 (4)C13—C141.381 (6)
S3—N21.644 (3)C13—H130.9300
S3—N11.655 (3)C14—C151.386 (5)
Cl1—C31.752 (4)C14—H140.9300
F1—C51.361 (5)C16—C211.373 (5)
N1—C11.300 (4)C16—C171.384 (5)
N2—C21.324 (5)C16—H160.9300
P1—C271.798 (3)C17—C181.376 (7)
P1—C211.799 (3)C17—H170.9300
P1—C151.802 (4)C18—C191.370 (7)
P1—C91.816 (3)C18—H180.9300
C1—C21.427 (5)C19—C201.368 (6)
C3—C81.393 (5)C19—H190.9300
C3—C41.394 (5)C20—C211.394 (5)
C4—C51.361 (6)C20—H200.9300
C4—H40.9300C22—C271.379 (5)
C5—C61.368 (6)C22—C231.380 (6)
C6—C71.375 (5)C22—H220.9300
C6—H60.9300C23—C241.349 (6)
C7—C81.401 (5)C23—H230.9300
C7—H70.9300C24—C251.391 (6)
C8—C91.503 (5)C24—H240.9300
C9—H9A0.9700C25—C261.388 (5)
C9—H9B0.9700C25—H250.9300
C10—C111.371 (6)C26—C271.400 (5)
C10—C151.395 (5)C26—H260.9300
S1i—Ni1—S1180.00 (4)C10—C11—H11119.8
S1i—Ni1—S2i93.18 (3)C12—C11—H11119.8
S1—Ni1—S2i86.82 (3)C13—C12—C11120.3 (4)
S1i—Ni1—S286.82 (3)C13—C12—H12119.9
S1—Ni1—S293.18 (3)C11—C12—H12119.9
S2i—Ni1—S2180.00 (8)C12—C13—C14120.3 (4)
C1—S1—Ni1103.26 (11)C12—C13—H13119.8
C2—S2—Ni1102.65 (12)C14—C13—H13119.8
N2—S3—N198.37 (16)C13—C14—C15119.4 (4)
C1—N1—S3106.9 (3)C13—C14—H14120.3
C2—N2—S3106.6 (3)C15—C14—H14120.3
C27—P1—C21109.46 (16)C14—C15—C10120.0 (3)
C27—P1—C15109.54 (16)C14—C15—P1120.6 (3)
C21—P1—C15109.54 (16)C10—C15—P1119.2 (3)
C27—P1—C9108.25 (16)C21—C16—C17119.6 (4)
C21—P1—C9109.81 (16)C21—C16—H16120.2
C15—P1—C9110.22 (16)C17—C16—H16120.2
N1—C1—C2114.5 (3)C18—C17—C16119.8 (4)
N1—C1—S1125.5 (3)C18—C17—H17120.1
C2—C1—S1120.1 (3)C16—C17—H17120.1
N2—C2—C1113.6 (3)C19—C18—C17120.9 (4)
N2—C2—S2125.7 (3)C19—C18—H18119.6
C1—C2—S2120.7 (3)C17—C18—H18119.6
C8—C3—C4121.8 (4)C20—C19—C18119.5 (4)
C8—C3—Cl1121.3 (3)C20—C19—H19120.2
C4—C3—Cl1116.8 (3)C18—C19—H19120.2
C5—C4—C3117.8 (4)C19—C20—C21120.3 (4)
C5—C4—H4121.1C19—C20—H20119.8
C3—C4—H4121.1C21—C20—H20119.8
F1—C5—C4117.8 (4)C16—C21—C20119.8 (4)
F1—C5—C6119.0 (4)C16—C21—P1122.2 (3)
C4—C5—C6123.2 (4)C20—C21—P1117.9 (3)
C5—C6—C7118.1 (4)C27—C22—C23119.8 (4)
C5—C6—H6120.9C27—C22—H22120.1
C7—C6—H6120.9C23—C22—H22120.1
C6—C7—C8122.0 (4)C24—C23—C22120.9 (4)
C6—C7—H7119.0C24—C23—H23119.6
C8—C7—H7119.0C22—C23—H23119.6
C3—C8—C7116.9 (3)C23—C24—C25120.7 (4)
C3—C8—C9122.8 (3)C23—C24—H24119.7
C7—C8—C9120.2 (3)C25—C24—H24119.7
C8—C9—P1112.3 (2)C26—C25—C24119.4 (4)
C8—C9—H9A109.2C26—C25—H25120.3
P1—C9—H9A109.2C24—C25—H25120.3
C8—C9—H9B109.2C25—C26—C27119.4 (4)
P1—C9—H9B109.2C25—C26—H26120.3
H9A—C9—H9B107.9C27—C26—H26120.3
C11—C10—C15119.5 (4)C22—C27—C26119.8 (3)
C11—C10—H10120.3C22—C27—P1120.8 (3)
C15—C10—H10120.3C26—C27—P1119.2 (3)
C10—C11—C12120.4 (4)
D—H···AD—HH···AD···AD—H···A
C9—H9A···S1ii0.972.713.635 (4)160
C9—H9B···Cl10.972.663.129 (4)110
C24—H24···N2iii0.932.613.401 (7)143
Ni1—S12.1842 (9)
Ni1—S22.1966 (9)
S1i—Ni1—S286.82 (3)
S1—Ni1—S293.18 (3)

Symmetry code: (i) .

Table 2

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
C9—H9A⋯S1ii0.972.713.635 (4)160
C9—H9B⋯Cl10.972.663.129 (4)110
C24—H24⋯N2iii0.932.613.401 (7)143

Symmetry codes: (ii) ; (iii) .

  4 in total

1.  Peculiar magnetic behavior in ion-pair complex [1-(4'-fluorobenzyl)pyridinium][Ni(mnt)2] (mnt2- = maleonitriledithiolate).

Authors:  Jingli Xie; Xiaoming Ren; You Song; Wenwei Zhang; Wenlong Liu; Cheng He; Qingjin Meng
Journal:  Chem Commun (Camb)       Date:  2002-10-21       Impact factor: 6.222

2.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

3.  Unusual magnetic properties of one-dimensional molecule-based magnets associated with a structural phase transition.

Authors:  Xiaoming Ren; Qingjin Meng; You Song; Changsheng Lu; Chuanjiang Hu; Xiaoyuan Chen
Journal:  Inorg Chem       Date:  2002-11-04       Impact factor: 5.165

4.  Theoretical studies on the magnetic switching controlled by stacking patterns of bis(maleonitriledithiolato) nickelate(III) dimers.

Authors:  Zhaoping Ni; Xiaoming Ren; Jing Ma; Jingli Xie; Chunlin Ni; Zhida Chen; Qingjin Meng
Journal:  J Am Chem Soc       Date:  2005-10-19       Impact factor: 15.419

  4 in total

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