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In the title compound, {NH4[Au(SCN)2]}n, the AuI atom is in a linear configuration with the coordinating S atoms. The extended structure can be described as a one-dimensional polymeric chain with alternating Au-Au bond distances of 3.1409 (3) and 3.1723 (3) Å.
Supporting information
CCDC reference: 298707
Key indicators
- Single-crystal X-ray study
- T = 150 K
- Mean (N-C) = 0.007 Å
- R factor = 0.022
- wR factor = 0.059
- Data-to-parameter ratio = 16.1
checkCIF/PLATON results
No syntax errors found
Alert level C
PLAT042_ALERT_1_C Calc. and Rep. MoietyFormula Strings Differ .... ?
0 ALERT level A = In general: serious problem
0 ALERT level B = Potentially serious problem
1 ALERT level C = Check and explain
0 ALERT level G = General alerts; check
1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data
0 ALERT type 2 Indicator that the structure model may be wrong or deficient
0 ALERT type 3 Indicator that the structure quality may be low
0 ALERT type 4 Improvement, methodology, query or suggestion
Data collection: SMART (Bruker, 2002); cell refinement: SAINT (Bruker, 2002); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Bruker, 2003); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL and DIAMOND (Brandenburg, 2005); software used to prepare material for publication: SHELXTL.
catena-Poly[ammonium [bis(thiocyanato)gold(I)](Au—Au)]
top
Crystal data top
(NH4N)[Au(NCS)2] | F(000) = 1184 |
Mr = 331.17 | Dx = 3.240 Mg m−3 |
Monoclinic, C2/c | Melting point: 164 ° with decomposition K |
Hall symbol: -C 2yc | Cu Kα radiation, λ = 1.54184 Å |
a = 12.9665 (2) Å | Cell parameters from 3756 reflections |
b = 6.3132 (1) Å | θ = 5.3–67.7° |
c = 17.6643 (3) Å | µ = 45.69 mm−1 |
β = 110.122 (1)° | T = 150 K |
V = 1357.74 (4) Å3 | Rod, colorless |
Z = 8 | 0.11 × 0.04 × 0.03 mm |
Data collection top
SMART6000 CCD diffractometer | 1209 independent reflections |
Radiation source: fine-focus sealed tube | 1123 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.029 |
Detector resolution: 0.83 pixels mm-1 | θmax = 67.7°, θmin = 5.3° |
ω scans | h = −15→15 |
Absorption correction: multi-scan (SADABS; Sheldrick, 2003) | k = −6→7 |
Tmin = 0.061, Tmax = 0.256 | l = −21→21 |
5457 measured reflections | |
Refinement top
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: mixed |
R[F2 > 2σ(F2)] = 0.022 | H-atom parameters constrained |
wR(F2) = 0.059 | w = 1/[σ2(Fo2) + (0.033P)2 + 4.3348P] where P = (Fo2 + 2Fc2)/3 |
S = 1.16 | (Δ/σ)max < 0.001 |
1209 reflections | Δρmax = 0.97 e Å−3 |
75 parameters | Δρmin = −1.58 e Å−3 |
0 restraints | Extinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.000284 (16) |
Special details top
Experimental. A suitable crystal was mounted on the tip of a glass fiber with paratone-N. The final unit cell is obtained from the refinement of the XYZ weighted
centroids of reflections above 20 σ(I). Note that the absorption correction parameters Tmin and Tmax also reflect beam
corrections, etc. As a result, the numerical values for Tmin and Tmax
may differ from expected values based solely absorption effects and crystal
size. |
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 | x | y | z | Uiso*/Ueq | |
N3 | 0.3265 (3) | 0.4904 (6) | 0.4413 (2) | 0.0247 (8) | |
H1 | 0.3677 | 0.6016 | 0.4700 | 0.037* | |
H2 | 0.3795 | 0.3984 | 0.4481 | 0.037* | |
H3 | 0.2768 | 0.4585 | 0.4629 | 0.037* | |
H4 | 0.2885 | 0.5604 | 0.3989 | 0.037* | |
Au1 | 0.5000 | 0.32757 (4) | 0.2500 | 0.01534 (14) | |
Au2 | 0.5000 | 0.83005 (4) | 0.2500 | 0.01348 (14) | |
S1 | 0.68661 (9) | 0.31698 (17) | 0.27506 (6) | 0.0211 (3) | |
S2 | 0.51549 (10) | 0.80341 (17) | 0.38350 (6) | 0.0226 (3) | |
N1 | 0.7635 (3) | 0.5370 (7) | 0.4234 (3) | 0.0287 (9) | |
N2 | 0.5183 (3) | 1.2261 (6) | 0.4365 (2) | 0.0235 (8) | |
C1 | 0.7301 (4) | 0.4525 (7) | 0.3623 (3) | 0.0190 (9) | |
C2 | 0.5166 (3) | 1.0562 (7) | 0.4128 (2) | 0.0145 (9) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
N3 | 0.028 (2) | 0.021 (2) | 0.0213 (19) | 0.0007 (16) | 0.0028 (16) | 0.0032 (16) |
Au1 | 0.0198 (2) | 0.0153 (2) | 0.00869 (19) | 0.000 | 0.00201 (12) | 0.000 |
Au2 | 0.01860 (19) | 0.0152 (2) | 0.00682 (18) | 0.000 | 0.00463 (12) | 0.000 |
S1 | 0.0214 (5) | 0.0229 (6) | 0.0191 (6) | 0.0008 (4) | 0.0070 (4) | −0.0029 (4) |
S2 | 0.0431 (7) | 0.0182 (5) | 0.0087 (5) | 0.0062 (5) | 0.0117 (5) | 0.0027 (4) |
N1 | 0.021 (2) | 0.034 (2) | 0.026 (2) | 0.0022 (17) | 0.0003 (18) | −0.0086 (18) |
N2 | 0.036 (2) | 0.025 (2) | 0.0115 (18) | 0.0018 (17) | 0.0104 (16) | −0.0011 (16) |
C1 | 0.011 (2) | 0.019 (2) | 0.026 (3) | 0.0030 (15) | 0.0039 (18) | 0.0024 (18) |
C2 | 0.017 (2) | 0.022 (2) | 0.0049 (19) | 0.0020 (15) | 0.0039 (16) | 0.0012 (16) |
Geometric parameters (Å, º) top
N3—H1 | 0.9211 | Au1—Au2 | 3.1723 (3) |
N3—H2 | 0.8757 | Au2—S2 | 2.3030 (10) |
N3—H3 | 0.8780 | S1—C1 | 1.680 (5) |
N3—H4 | 0.8635 | S2—C2 | 1.676 (4) |
Au1—S1 | 2.3062 (11) | N1—C1 | 1.148 (6) |
Au1—Au2i | 3.1409 (3) | N2—C2 | 1.149 (6) |
| | | |
H1—N3—H2 | 98.7 | Au2i—Au1—Au2 | 180.0 |
H1—N3—H3 | 108.0 | S2ii—Au2—S2 | 171.63 (5) |
H2—N3—H3 | 116.6 | S2—Au2—Au1iii | 94.19 (3) |
H1—N3—H4 | 97.9 | C1—S1—Au1 | 99.22 (15) |
H2—N3—H4 | 130.2 | C2—S2—Au2 | 103.59 (15) |
H3—N3—H4 | 102.0 | N1—C1—S1 | 176.6 (4) |
S1—Au1—S1ii | 176.68 (5) | N2—C2—S2 | 176.8 (4) |
S1—Au1—Au2i | 88.34 (3) | | |
| | | |
Au2i—Au1—S1—C1 | −121.37 (16) | Au1iii—Au2—S2—C2 | 1.00 (16) |
Au2—Au1—S1—C1 | 58.63 (16) | | |
Symmetry codes: (i) x, y−1, z; (ii) −x+1, y, −z+1/2; (iii) x, y+1, z. |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
N3—H1···N2iv | 0.92 | 2.10 | 2.987 (6) | 161 |
N3—H2···N2i | 0.88 | 2.17 | 3.020 (6) | 163 |
N3—H3···N1v | 0.88 | 2.24 | 3.004 (6) | 145 |
Symmetry codes: (i) x, y−1, z; (iv) −x+1, −y+2, −z+1; (v) −x+1, −y+1, −z+1. |
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