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The Au atom in the title compound, [Au(CH3)2(C13H10NO)], has a square-planar coordination geometry. The mol­ecule is located on a crystallographic mirror plane. The phenolate ring is disordered over two equally occupied positions. The mol­ecules are packed in infinite stacks parallel to the b axis, with an Au...Au distance of 4.2106 (4) Å.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807060709/bt2619sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807060709/bt2619Isup2.hkl
Contains datablock I

CCDC reference: 672752

Key indicators

  • Single-crystal X-ray study
  • T = 150 K
  • Mean [sigma](C-C) = 0.004 Å
  • Disorder in main residue
  • R factor = 0.012
  • wR factor = 0.027
  • Data-to-parameter ratio = 12.6

checkCIF/PLATON results

No syntax errors found



Alert level A PLAT222_ALERT_3_A Large Non-Solvent H Ueq(max)/Ueq(min) ... 5.38 Ratio
Author Response: The atom is disordered

Alert level B PLAT220_ALERT_2_B Large Non-Solvent C Ueq(max)/Ueq(min) ... 4.22 Ratio
Alert level C PLAT062_ALERT_4_C Rescale T(min) & T(max) by ..................... 0.93 PLAT213_ALERT_2_C Atom C12 has ADP max/min Ratio ............. 3.50 prola PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for Au1 PLAT250_ALERT_2_C Large U3/U1 Ratio for Average U(i,j) Tensor .... 2.96 PLAT301_ALERT_3_C Main Residue Disorder ......................... 22.00 Perc.
Alert level G ABSTM02_ALERT_3_G When printed, the submitted absorption T values will be replaced by the scaled T values. Since the ratio of scaled T's is identical to the ratio of reported T values, the scaling does not imply a change to the absorption corrections used in the study. Ratio of Tmax expected/reported 0.929 Tmax scaled 0.524 Tmin scaled 0.422
1 ALERT level A = In general: serious problem 1 ALERT level B = Potentially serious problem 5 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 4 ALERT type 2 Indicator that the structure model may be wrong or deficient 3 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

The title compound has molecular structure constructed from neutral molecules (CH3)2Au(C13H10NO). The gold atom in the molecule has a slightly distorted square planar configuration formed by oxygen and nitrogen atoms of salicilaldimine ligand, and two carbon atoms of methyl groups (Fig. 1). In the coordination square, Au—O and Au—N distances differ slightly, and O—Au—N angle is very close to 90°. The values of Au—CH3 bonds are typical for dimethylgold(III) derivatives (Shibata et al., 1990; Bessonov, Baidina et al., 2007). The salicylaldimine fragment is located on a mirror plane, however carbon atoms C5, C6, C7, C8 and C9 are disordered. The planes of salycilaldimine and phenyl ring are nearly perpendicular (the angle is about 91°). In the crystal, molecules are packed in infinite stacks along the monoclinic axis with the shortest Au···Au distance of 4.2106 (4) Å and Au—Au—Au angle of 121.173 (8)° (Fig. 2). The oxygen atom is involved in intermolecular O···H—C interactions with O···C distances of 3.291 (3) Å. The shortest intermolecular H···H distance in the crystal is about 2.5 Å.

Related literature top

Dimethylgold(III) derivatives are used in metal-organic chemical vapor deposition processes because of their volatility and thermal stability (Larson et al., 1987; Semyannikov et al., 2006; Bessonov, Morozova et al., 2007; Bessonov, Baidina et al., 2007). For a similar structure, see: Shibata et al. (1990). For literature related to the synthesis, see: Bessonov et al. (2008); Murray et al. (1973).

Experimental top

Sodium bicarbonate, NaHCO3, and dimethylgold(III) iodide, [(CH3)2AuI]2, (prepared as described in Bessonov et al., 2008) were added to a solution of N-phenylsalicylaldimine in methanol. The mixture was stirred for 6 h in an argon flow. Then, the methanol was removed in vacuum and the residue was redissolved in hexane. The hexane solution was filtered and the volatile components were removed in vacuum. The complex was purified by recrystallization from hexane at -10°C. Pale yellow crystals suitable for X-ray analysis were formed in yield of 80%. The melting point of the complex was 147–150°C (154°C from Murray et al., 1973). The product is stable to air and moisture and soluble in most common organic solvents.

Refinement top

H atoms were were refined with fixed individual displacement parameters [U(H) = 1.2 Ueq(C) using a riding model with Caromatic—H = 0.95 Å and Cmethyl—H = 0.98 Å. The phenolic ring and the methyl H atoms are disordered over two equally occupied positions.

Computing details top

Data collection: APEX2 (Bruker, 2004); cell refinement: SAINT (Bruker, 2004); data reduction: SAINT (Bruker, 2004); program(s) used to solve structure: SHELXTL (Bruker, 2004); program(s) used to refine structure: SHELXTL (Bruker, 2004); molecular graphics: POV-RAY (Cason, 2002); software used to prepare material for publication: SHELXTL (Bruker, 2004).

Figures top
[Figure 1] Fig. 1. Plot of Me2Au(Sal=N—Ph) molecule showing the atom numbering for the core atoms. Displacement ellipsoids are drawn at the 50% probability level. Only one set of the two disordered atoms is shown.
[Figure 2] Fig. 2. A packing diagram of the Me2Au(Sal=N—Ph) structure, viewed along the b axis. H atoms omitted for clarity. Only one set of the two disordered atoms is shown.
Dimethyl[2-(phenyliminomethyl)phenolato-κ2N,O]gold(III) top
Crystal data top
[Au(CH3)2(C13H10NO)]F(000) = 400
Mr = 423.25Dx = 2.058 Mg m3
Monoclinic, P21/mMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybCell parameters from 3995 reflections
a = 8.5316 (10) Åθ = 2.4–28.3°
b = 7.3356 (7) ŵ = 10.76 mm1
c = 11.1180 (13) ÅT = 150 K
β = 101.006 (3)°Needle, pale yellow
V = 683.02 (13) Å30.25 × 0.06 × 0.06 mm
Z = 2
Data collection top
Bruker–Nonius X8 APEX CCD area-detector
diffractometer
1506 independent reflections
Radiation source: fine-focus sealed tube1423 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.018
Detector resolution: 25 pixels mm-1θmax = 26.4°, θmin = 1.9°
ϕ scansh = 1010
Absorption correction: multi-scan
(SADABS; Bruker, 2004)
k = 69
Tmin = 0.454, Tmax = 0.565l = 1313
4954 measured 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)] = 0.012Hydrogen site location: difference Fourier map
wR(F2) = 0.027H-atom parameters constrained
S = 1.11 w = 1/[σ2(Fo2) + (0.0113P)2 + 0.2414P]
where P = (Fo2 + 2Fc2)/3
1506 reflections(Δ/σ)max = 0.001
120 parametersΔρmax = 0.43 e Å3
0 restraintsΔρmin = 0.52 e Å3
Crystal data top
[Au(CH3)2(C13H10NO)]V = 683.02 (13) Å3
Mr = 423.25Z = 2
Monoclinic, P21/mMo Kα radiation
a = 8.5316 (10) ŵ = 10.76 mm1
b = 7.3356 (7) ÅT = 150 K
c = 11.1180 (13) Å0.25 × 0.06 × 0.06 mm
β = 101.006 (3)°
Data collection top
Bruker–Nonius X8 APEX CCD area-detector
diffractometer
1506 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2004)
1423 reflections with I > 2σ(I)
Tmin = 0.454, Tmax = 0.565Rint = 0.018
4954 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0120 restraints
wR(F2) = 0.027H-atom parameters constrained
S = 1.11Δρmax = 0.43 e Å3
1506 reflectionsΔρmin = 0.52 e Å3
120 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*/UeqOcc. (<1)
Au10.935702 (14)0.25000.069963 (11)0.02283 (5)
N11.1812 (3)0.25000.0660 (2)0.0256 (6)
O10.8825 (3)0.25000.12028 (19)0.0255 (5)
C130.9623 (4)0.25000.2555 (3)0.0393 (10)
H13A0.86830.30610.27900.059*0.50
H13B1.05790.31960.29110.059*0.50
H13C0.97330.12430.28570.059*0.50
C110.9822 (4)0.25000.1954 (3)0.0265 (7)
C51.2359 (5)0.2098 (5)0.0345 (4)0.0203 (14)0.50
H51.34540.17700.02320.024*0.50
C120.6969 (5)0.25000.0668 (4)0.086 (2)
H12A0.66300.37260.08570.129*0.50
H12B0.67250.16360.12780.129*0.50
H12C0.64020.21380.01480.129*0.50
C11.3007 (4)0.25000.1778 (3)0.0263 (7)
C41.5304 (4)0.25000.3890 (3)0.0367 (9)
H41.61080.25000.46100.044*
C21.3560 (3)0.0877 (4)0.2304 (2)0.0438 (7)
H21.31560.02460.19470.053*
C31.4724 (4)0.0896 (4)0.3371 (3)0.0483 (8)
H31.51170.02240.37400.058*
C61.1492 (5)0.2099 (6)0.1589 (4)0.0217 (15)0.50
C100.9187 (4)0.25000.3223 (3)0.0338 (8)
H100.80880.27670.34980.041*0.50
C91.0136 (6)0.2117 (7)0.4081 (4)0.0292 (18)0.50
H90.96540.20100.49220.035*0.50
C81.1776 (6)0.1888 (7)0.3728 (4)0.0379 (15)0.50
H81.24330.17380.43210.045*0.50
C71.2419 (6)0.1884 (6)0.2503 (4)0.0320 (13)0.50
H71.35400.17300.22570.038*0.50
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Au10.01707 (7)0.03630 (8)0.01489 (7)0.0000.00249 (5)0.000
N10.0208 (14)0.0411 (17)0.0138 (13)0.0000.0006 (11)0.000
O10.0201 (11)0.0402 (13)0.0153 (11)0.0000.0011 (9)0.000
C130.030 (2)0.073 (3)0.0160 (18)0.0000.0060 (15)0.000
C110.0248 (17)0.0351 (19)0.0192 (17)0.0000.0032 (14)0.000
C50.0171 (18)0.020 (4)0.023 (2)0.0005 (15)0.0014 (15)0.0012 (16)
C120.018 (2)0.213 (7)0.027 (2)0.0000.0045 (17)0.000
C10.0156 (15)0.049 (2)0.0143 (16)0.0000.0021 (13)0.000
C40.0229 (18)0.067 (3)0.0172 (17)0.0000.0029 (14)0.000
C20.0474 (17)0.0474 (17)0.0285 (14)0.0204 (13)0.0134 (12)0.0121 (12)
C30.0539 (18)0.0532 (18)0.0302 (15)0.0070 (15)0.0111 (13)0.0173 (14)
C60.025 (2)0.024 (4)0.0152 (18)0.0032 (17)0.0019 (15)0.0001 (17)
C100.0287 (19)0.053 (2)0.0172 (17)0.0000.0018 (14)0.000
C90.039 (2)0.031 (6)0.0158 (19)0.001 (2)0.0012 (17)0.0008 (19)
C80.036 (3)0.060 (4)0.021 (2)0.003 (2)0.014 (2)0.004 (2)
C70.024 (2)0.047 (3)0.026 (2)0.0008 (19)0.0071 (19)0.0023 (19)
Geometric parameters (Å, º) top
Au1—C122.030 (4)C8—C71.368 (7)
Au1—C132.031 (3)C13—H13A0.9800
Au1—O12.077 (2)C13—H13B0.9800
Au1—N12.104 (3)C13—H13C0.9800
N1—C51.324 (5)C12—H12A0.9800
N1—C11.449 (4)C12—H12B0.9800
O1—C111.301 (4)C12—H12C0.9800
C11—C101.411 (5)C5—H50.9500
C11—C61.436 (5)C4—H40.9500
C5—C61.438 (6)C2—H20.9500
C1—C21.369 (3)C3—H30.9500
C4—C31.361 (4)C10—H100.9500
C2—C31.392 (4)C9—H90.9500
C6—C71.412 (6)C8—H80.9500
C10—C91.393 (6)C7—H70.9500
C9—C81.389 (7)
C12—Au1—C1386.27 (16)H13A—C13—H13B109.5
C12—Au1—O187.62 (14)Au1—C13—H13C109.5
C13—Au1—O1173.89 (11)H13A—C13—H13C109.5
C12—Au1—N1177.84 (14)H13B—C13—H13C109.5
C13—Au1—N195.89 (13)N1—C5—H5116.1
O1—Au1—N190.22 (9)C6—C5—H5116.1
C5—N1—C1114.9 (3)Au1—C12—H12A109.5
C5—N1—Au1122.0 (2)Au1—C12—H12B109.5
C1—N1—Au1121.5 (2)H12A—C12—H12B109.5
C11—O1—Au1127.7 (2)Au1—C12—H12C109.5
O1—C11—C10117.9 (3)H12A—C12—H12C109.5
C10—C11—C6117.0 (3)H12B—C12—H12C109.5
O1—C11—C6123.7 (3)C3—C4—H4120.2
N1—C5—C6127.8 (4)C1—C2—H2120.5
C2—C1—N1119.70 (16)C3—C2—H2120.5
C1—C2—C3119.2 (3)C4—C3—H3119.6
C4—C3—C2120.8 (3)C2—C3—H3119.6
C7—C6—C11118.9 (4)C9—C10—H10119.2
C7—C6—C5115.8 (4)C11—C10—H10119.2
C11—C6—C5124.9 (4)C8—C9—H9119.5
C9—C10—C11121.4 (4)C10—C9—H9119.5
C10—C9—C8121.2 (4)C7—C8—H8120.9
C7—C8—C9118.3 (4)C9—C8—H8120.9
C8—C7—C6122.8 (4)C8—C7—H7118.5
Au1—C13—H13A109.5C6—C7—H7118.5
Au1—C13—H13B109.5

Experimental details

Crystal data
Chemical formula[Au(CH3)2(C13H10NO)]
Mr423.25
Crystal system, space groupMonoclinic, P21/m
Temperature (K)150
a, b, c (Å)8.5316 (10), 7.3356 (7), 11.1180 (13)
β (°) 101.006 (3)
V3)683.02 (13)
Z2
Radiation typeMo Kα
µ (mm1)10.76
Crystal size (mm)0.25 × 0.06 × 0.06
Data collection
DiffractometerBruker–Nonius X8 APEX CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Bruker, 2004)
Tmin, Tmax0.454, 0.565
No. of measured, independent and
observed [I > 2σ(I)] reflections
4954, 1506, 1423
Rint0.018
(sin θ/λ)max1)0.625
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.012, 0.027, 1.11
No. of reflections1506
No. of parameters120
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.43, 0.52

Computer programs: APEX2 (Bruker, 2004), SAINT (Bruker, 2004), SHELXTL (Bruker, 2004), POV-RAY (Cason, 2002).

Selected bond lengths (Å) top
Au1—C122.030 (4)Au1—O12.077 (2)
Au1—C132.031 (3)Au1—N12.104 (3)
 

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