Diiodido(1,10-phenanthroline-κN,N')platinum(II).

In the title complex, [PtI(2)(C(12)H(8)N(2))], the Pt(2+) ion is four-coordinated in a slightly distorted square-planar environment by two N atoms of the chelating 1,10-phenanthroline ligand and two iodide ions. The nearly planar mol-ecules, with a maximum deviation of 0.170 (3) Å from the least-squares plane, are stacked in columns along the c axis with a Pt⋯Pt distance of 4.8510 (6) Å. In the column, π-π inter-actions between adjacent six-membered rings are present, the shortest centroid-centroid distance being 3.703 (5) Å.

Related literature

For the syntheses of [PtX 2(phen)] (phen = 1,10-phenanthroline; X = Cl, Br or I), see: Hodges & Rund (1975 ▶). For the crystal structure of yellow [PtCl2(phen)] which is isotypic to the title complex, see: Grzesiak & Matzger (2007 ▶).

Experimental

Crystal data

[PtI2(C12H8N2)]

M = 629.09

Monoclinic,

a = 10.3284 (9) Å

b = 17.9462 (16) Å

c = 7.3833 (7) Å

β = 108.569 (2)°

V = 1297.3 (2) Å3

Z = 4

Mo Kα radiation

μ = 15.55 mm−1

T = 200 K

0.32 × 0.13 × 0.08 mm

Data collection

Bruker SMART 1000 CCD diffractometer

Absorption correction: multi-scan (SADABS; Bruker, 2000 ▶) T min = 0.422, T max = 1.000

7331 measured reflections

2284 independent reflections

2110 reflections with I > 2σ(I)

R int = 0.033

Refinement

R[F 2 > 2σ(F 2)] = 0.033

wR(F 2) = 0.084

S = 1.06

2284 reflections

154 parameters

H-atom parameters constrained

Δρmax = 3.05 e Å−3

Δρmin = −1.40 e Å−3

Data collection: SMART (Bruker, 2000 ▶); cell refinement: SAINT (Bruker, 2000 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶) and PLATON (Spek, 2009 ▶); software used to prepare material for publication: SHELXL97.

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809053100/ng2700sup1.cif

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809053100/ng2700Isup2.hkl

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

[PtI2(C12H8N2)]	F(000) = 1112
Mr = 629.09	Dx = 3.221 Mg m−3
Monoclinic, P21/c	Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc	Cell parameters from 5463 reflections
a = 10.3284 (9) Å	θ = 2.3–28.2°
b = 17.9462 (16) Å	µ = 15.55 mm−1
c = 7.3833 (7) Å	T = 200 K
β = 108.569 (2)°	Needle, yellow
V = 1297.3 (2) Å3	0.32 × 0.13 × 0.08 mm
Z = 4

Bruker SMART 1000 CCD diffractometer	2284 independent reflections
Radiation source: fine-focus sealed tube	2110 reflections with I > 2σ(I)
graphite	Rint = 0.033
φ and ω scans	θmax = 25.1°, θmin = 2.1°
Absorption correction: multi-scan (SADABS; Bruker, 2000)	h = −11→12
Tmin = 0.422, Tmax = 1.000	k = −21→21
7331 measured reflections	l = −8→8

Refinement on F2	Primary atom site location: structure-invariant direct methods
Least-squares matrix: full	Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.033	Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.084	H-atom parameters constrained
S = 1.06	w = 1/[σ2(Fo2) + (0.0524P)2 + 0.9657P] where P = (Fo2 + 2Fc2)/3
2284 reflections	(Δ/σ)max < 0.001
154 parameters	Δρmax = 3.05 e Å−3
0 restraints	Δρmin = −1.40 e Å−3

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.

	x	y	z	Uiso*/Ueq
Pt1	0.71220 (3)	0.337678 (16)	0.39502 (4)	0.02011 (13)
I1	0.74244 (6)	0.48072 (3)	0.41617 (8)	0.03146 (17)
I2	0.45788 (6)	0.35783 (3)	0.20604 (9)	0.03744 (18)
N1	0.7037 (6)	0.2230 (4)	0.3858 (8)	0.0245 (15)
N2	0.9082 (6)	0.3142 (4)	0.5563 (9)	0.0219 (13)
C1	0.6012 (9)	0.1789 (5)	0.2965 (12)	0.034 (2)
H1	0.5167	0.2005	0.2237	0.041*
C2	0.6130 (9)	0.1009 (5)	0.3056 (13)	0.035 (2)
H2	0.5376	0.0709	0.2367	0.042*
C3	0.7305 (10)	0.0681 (6)	0.4114 (11)	0.036 (2)
H3	0.7375	0.0153	0.4195	0.044*
C4	0.8426 (9)	0.1132 (4)	0.5097 (12)	0.0291 (19)
C5	0.9726 (10)	0.0861 (5)	0.6267 (13)	0.034 (2)
H5	0.9862	0.0338	0.6419	0.041*
C6	1.0755 (9)	0.1317 (5)	0.7155 (13)	0.0317 (19)
H6	1.1602	0.1114	0.7921	0.038*
C7	1.0598 (8)	0.2110 (4)	0.6964 (11)	0.0248 (17)
C8	1.1647 (8)	0.2622 (5)	0.7825 (11)	0.0311 (19)
H8	1.2519	0.2453	0.8600	0.037*
C9	1.1388 (9)	0.3359 (4)	0.7527 (12)	0.0300 (19)
H9	1.2091	0.3708	0.8101	0.036*
C10	1.0137 (8)	0.3614 (5)	0.6417 (11)	0.0261 (17)
H10	0.9999	0.4135	0.6236	0.031*
C11	0.9351 (8)	0.2394 (4)	0.5838 (10)	0.0208 (16)
C12	0.8236 (8)	0.1915 (4)	0.4917 (11)	0.0233 (17)

	U11	U22	U33	U12	U13	U23
Pt1	0.0168 (2)	0.0209 (2)	0.0209 (2)	−0.00133 (10)	0.00349 (14)	−0.00034 (10)
I1	0.0309 (3)	0.0217 (3)	0.0393 (3)	0.0010 (2)	0.0077 (3)	0.0001 (2)
I2	0.0184 (3)	0.0439 (4)	0.0433 (4)	0.0001 (2)	0.0004 (2)	0.0026 (3)
N1	0.024 (4)	0.028 (4)	0.023 (3)	−0.004 (3)	0.010 (3)	−0.002 (3)
N2	0.018 (4)	0.025 (3)	0.022 (3)	0.001 (3)	0.006 (3)	0.001 (3)
C1	0.031 (5)	0.040 (5)	0.032 (5)	−0.019 (4)	0.010 (4)	−0.012 (4)
C2	0.030 (5)	0.034 (5)	0.041 (5)	−0.015 (4)	0.011 (4)	−0.007 (4)
C3	0.059 (7)	0.026 (5)	0.031 (5)	−0.006 (4)	0.025 (5)	−0.005 (3)
C4	0.043 (5)	0.021 (4)	0.031 (4)	−0.005 (4)	0.023 (4)	0.001 (3)
C5	0.048 (6)	0.024 (5)	0.038 (5)	0.009 (4)	0.023 (5)	0.002 (4)
C6	0.028 (5)	0.032 (5)	0.038 (5)	0.003 (4)	0.014 (4)	0.004 (4)
C7	0.019 (4)	0.030 (4)	0.027 (4)	0.007 (3)	0.009 (3)	0.003 (3)
C8	0.020 (4)	0.046 (5)	0.025 (4)	0.010 (4)	0.005 (3)	0.006 (4)
C9	0.026 (5)	0.033 (5)	0.025 (4)	−0.005 (3)	0.000 (4)	−0.001 (3)
C10	0.017 (4)	0.023 (4)	0.032 (4)	−0.008 (3)	−0.001 (3)	−0.003 (3)
C11	0.024 (4)	0.019 (4)	0.021 (4)	−0.003 (3)	0.010 (3)	0.000 (3)
C12	0.033 (5)	0.021 (4)	0.022 (4)	−0.001 (3)	0.016 (4)	0.003 (3)

Pt1—N2	2.039 (6)	C4—C12	1.419 (11)
Pt1—N1	2.060 (7)	C4—C5	1.431 (13)
Pt1—I2	2.5774 (7)	C5—C6	1.337 (12)
Pt1—I1	2.5847 (6)	C5—H5	0.9500
N1—C1	1.319 (10)	C6—C7	1.434 (11)
N1—C12	1.360 (10)	C6—H6	0.9500
N2—C10	1.365 (10)	C7—C11	1.389 (11)
N2—C11	1.374 (10)	C7—C8	1.407 (12)
C1—C2	1.405 (13)	C8—C9	1.354 (12)
C1—H1	0.9500	C8—H8	0.9500
C2—C3	1.351 (13)	C9—C10	1.369 (12)
C2—H2	0.9500	C9—H9	0.9500
C3—C4	1.410 (12)	C10—H10	0.9500
C3—H3	0.9500	C11—C12	1.423 (11)
N2—Pt1—N1	80.6 (2)	C6—C5—C4	122.3 (8)
N2—Pt1—I2	175.02 (17)	C6—C5—H5	118.9
N1—Pt1—I2	95.57 (17)	C4—C5—H5	118.9
N2—Pt1—I1	95.23 (18)	C5—C6—C7	120.8 (8)
N1—Pt1—I1	175.72 (17)	C5—C6—H6	119.6
I2—Pt1—I1	88.63 (2)	C7—C6—H6	119.6
C1—N1—C12	118.5 (8)	C11—C7—C8	117.7 (7)
C1—N1—Pt1	129.5 (6)	C11—C7—C6	118.5 (7)
C12—N1—Pt1	112.1 (5)	C8—C7—C6	123.8 (7)
C10—N2—C11	116.4 (7)	C9—C8—C7	118.7 (8)
C10—N2—Pt1	129.8 (5)	C9—C8—H8	120.6
C11—N2—Pt1	113.8 (5)	C7—C8—H8	120.6
N1—C1—C2	122.1 (9)	C8—C9—C10	121.5 (8)
N1—C1—H1	119.0	C8—C9—H9	119.2
C2—C1—H1	119.0	C10—C9—H9	119.2
C3—C2—C1	120.6 (8)	N2—C10—C9	122.1 (8)
C3—C2—H2	119.7	N2—C10—H10	118.9
C1—C2—H2	119.7	C9—C10—H10	118.9
C2—C3—C4	119.2 (9)	N2—C11—C7	123.5 (7)
C2—C3—H3	120.4	N2—C11—C12	115.2 (7)
C4—C3—H3	120.4	C7—C11—C12	121.3 (7)
C3—C4—C12	117.0 (8)	N1—C12—C4	122.6 (7)
C3—C4—C5	125.0 (8)	N1—C12—C11	118.2 (7)
C12—C4—C5	117.9 (7)	C4—C12—C11	119.1 (7)
N2—Pt1—N1—C1	−178.5 (7)	Pt1—N2—C10—C9	177.2 (6)
I2—Pt1—N1—C1	4.8 (7)	C8—C9—C10—N2	0.4 (13)
N2—Pt1—N1—C12	2.5 (5)	C10—N2—C11—C7	2.1 (10)
I2—Pt1—N1—C12	−174.3 (4)	Pt1—N2—C11—C7	−176.9 (6)
N1—Pt1—N2—C10	179.0 (7)	C10—N2—C11—C12	−179.5 (6)
I1—Pt1—N2—C10	0.1 (7)	Pt1—N2—C11—C12	1.6 (8)
N1—Pt1—N2—C11	−2.2 (5)	C8—C7—C11—N2	−1.6 (11)
I1—Pt1—N2—C11	178.8 (4)	C6—C7—C11—N2	179.6 (7)
C12—N1—C1—C2	−0.9 (11)	C8—C7—C11—C12	−179.9 (7)
Pt1—N1—C1—C2	−179.9 (6)	C6—C7—C11—C12	1.2 (10)
N1—C1—C2—C3	1.6 (12)	C1—N1—C12—C4	0.0 (10)
C1—C2—C3—C4	−1.4 (12)	Pt1—N1—C12—C4	179.2 (5)
C2—C3—C4—C12	0.5 (11)	C1—N1—C12—C11	178.4 (7)
C2—C3—C4—C5	179.9 (8)	Pt1—N1—C12—C11	−2.4 (8)
C3—C4—C5—C6	179.5 (7)	C3—C4—C12—N1	0.2 (10)
C12—C4—C5—C6	−1.1 (12)	C5—C4—C12—N1	−179.3 (7)
C4—C5—C6—C7	−0.2 (12)	C3—C4—C12—C11	−178.2 (7)
C5—C6—C7—C11	0.1 (11)	C5—C4—C12—C11	2.4 (10)
C5—C6—C7—C8	−178.6 (8)	N2—C11—C12—N1	0.6 (10)
C11—C7—C8—C9	0.4 (11)	C7—C11—C12—N1	179.1 (6)
C6—C7—C8—C9	179.2 (7)	N2—C11—C12—C4	179.0 (6)
C7—C8—C9—C10	0.1 (12)	C7—C11—C12—C4	−2.5 (10)
C11—N2—C10—C9	−1.5 (11)

Pt1—N2	2.039 (6)
Pt1—N1	2.060 (7)
Pt1—I2	2.5774 (7)
Pt1—I1	2.5847 (6)

N2—Pt1—N1

80.6 (2)