The asymmetric unit of the title compound, [Co(NH
3)
6][Mn(CN)
6], contains one Co and one Mn atom, both lying on threefold inversion axes, and one NH
3 and one CN group. The octahedral environments around Co
II and Mn
II are generated by symmetry and show very slight deviations from ideal geometry. A three-dimensional network is created by N—H

N hydrogen bonds.
Supporting information
Key indicators
- Single-crystal X-ray study
- T = 100 K
- Mean
(N-C) = 0.003 Å
- R factor = 0.025
- wR factor = 0.071
- Data-to-parameter ratio = 19.6
checkCIF/PLATON results
No syntax errors found
Alert level B
PLAT232_ALERT_2_B Hirshfeld Test Diff (M-X) Mn1 -- C2 .. 11.58 su
0 ALERT level A = In general: serious problem
1 ALERT level B = Potentially serious problem
0 ALERT level C = Check and explain
0 ALERT level G = General alerts; check
0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data
1 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
0 ALERT type 5 Informative message, check
Equimolar amounts of K3[Mn(CN)6] and [Co(NH3)6]Cl3 were dissolved in
water, added together and allowed to stand. Orange crystals separated out
after a few days.
Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT-Plus (Bruker, 2004); data reduction: SAINT-Plus and XPREP (Bruker, 2004); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg & Putz, 2005); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008) and WinGX (Farrugia, 1999).
Hexaamminecobalt(III) hexacyanidomanganate(III)
top
Crystal data top
[Co(NH3)6][Mn(CN)6] | Dx = 1.653 Mg m−3 |
Mr = 372.19 | Mo Kα radiation, λ = 0.71069 Å |
Trigonal, R3 | Cell parameters from 1532 reflections |
Hall symbol: -R 3 | θ = 2.9–28.3° |
a = 10.963 (5) Å | µ = 1.96 mm−1 |
c = 10.779 (5) Å | T = 100 K |
V = 1121.9 (9) Å3 | Cuboid, orange |
Z = 3 | 0.35 × 0.26 × 0.25 mm |
F(000) = 570 | |
Data collection top
Bruker SMART APEXII CCD area-detector diffractometer | 497 reflections with I > 2σ(I) |
ϕ and ω scans | Rint = 0.038 |
Absorption correction: multi-scan (SADABS; Bruker, 2004) | θmax = 28.3°, θmin = 2.9° |
Tmin = 0.546, Tmax = 0.614 | h = −12→14 |
3602 measured reflections | k = −14→9 |
628 independent reflections | l = −10→14 |
Refinement top
Refinement on F2 | 0 restraints |
Least-squares matrix: full | H-atom parameters constrained |
R[F2 > 2σ(F2)] = 0.025 | w = 1/[σ2(Fo2) + (0.0379P)2 + 3.8029P] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.071 | (Δ/σ)max < 0.001 |
S = 0.93 | Δρmax = 0.29 e Å−3 |
628 reflections | Δρmin = −0.43 e Å−3 |
32 parameters | |
Crystal data top
[Co(NH3)6][Mn(CN)6] | Z = 3 |
Mr = 372.19 | Mo Kα radiation |
Trigonal, R3 | µ = 1.96 mm−1 |
a = 10.963 (5) Å | T = 100 K |
c = 10.779 (5) Å | 0.35 × 0.26 × 0.25 mm |
V = 1121.9 (9) Å3 | |
Data collection top
Bruker SMART APEXII CCD area-detector diffractometer | 628 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2004) | 497 reflections with I > 2σ(I) |
Tmin = 0.546, Tmax = 0.614 | Rint = 0.038 |
3602 measured reflections | |
Refinement top
R[F2 > 2σ(F2)] = 0.025 | 0 restraints |
wR(F2) = 0.071 | H-atom parameters constrained |
S = 0.93 | Δρmax = 0.29 e Å−3 |
628 reflections | Δρmin = −0.43 e Å−3 |
32 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. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | |
Co1 | 0 | 0 | 0 | 0.00732 (17) | |
Mn1 | 0.3333 | 0.6667 | 0.1667 | 0.00607 (17) | |
N1 | −0.02748 (15) | 0.13048 (15) | −0.10659 (13) | 0.0107 (3) | |
H1A | 0.0238 | 0.2179 | −0.0777 | 0.016* | |
H1B | −0.1181 | 0.1061 | −0.1065 | 0.016* | |
H1C | −0.0006 | 0.1264 | −0.1837 | 0.016* | |
C2 | 0.31385 (18) | 0.80238 (18) | 0.06080 (16) | 0.0119 (3) | |
N2 | 0.30018 (17) | 0.87891 (17) | −0.00283 (15) | 0.0184 (4) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Co1 | 0.0076 (2) | 0.0076 (2) | 0.0067 (3) | 0.00381 (10) | 0 | 0 |
Mn1 | 0.0064 (2) | 0.0064 (2) | 0.0055 (3) | 0.00318 (10) | 0 | 0 |
N1 | 0.0117 (7) | 0.0099 (7) | 0.0111 (7) | 0.0058 (6) | 0.0007 (5) | 0.0010 (5) |
C2 | 0.0108 (8) | 0.0144 (8) | 0.0115 (8) | 0.0070 (7) | 0.0001 (6) | −0.0026 (6) |
N2 | 0.0200 (8) | 0.0248 (9) | 0.0159 (7) | 0.0152 (7) | 0.0014 (6) | 0.0013 (6) |
Geometric parameters (Å, º) top
Co1—N1i | 1.9718 (16) | Mn1—C2vii | 1.9696 (19) |
Co1—N1ii | 1.9718 (16) | Mn1—C2viii | 1.9696 (19) |
Co1—N1iii | 1.9718 (15) | Mn1—C2ix | 1.9696 (19) |
Co1—N1iv | 1.9718 (15) | Mn1—C2x | 1.9696 (19) |
Co1—N1 | 1.9718 (15) | N1—H1A | 0.89 |
Co1—N1v | 1.9718 (15) | N1—H1B | 0.89 |
Mn1—C2vi | 1.9696 (19) | N1—H1C | 0.89 |
Mn1—C2 | 1.9696 (19) | C2—N2 | 1.150 (2) |
| | | |
N1i—Co1—N1ii | 180.00 (7) | C2—Mn1—C2viii | 89.80 (7) |
N1i—Co1—N1iii | 89.47 (6) | C2vii—Mn1—C2viii | 89.80 (7) |
N1ii—Co1—N1iii | 90.53 (6) | C2vi—Mn1—C2ix | 89.80 (7) |
N1i—Co1—N1iv | 89.47 (6) | C2—Mn1—C2ix | 90.20 (7) |
N1ii—Co1—N1iv | 90.53 (6) | C2vii—Mn1—C2ix | 180 |
N1iii—Co1—N1iv | 89.47 (6) | C2viii—Mn1—C2ix | 90.20 (7) |
N1i—Co1—N1 | 90.53 (6) | C2vi—Mn1—C2x | 89.80 (7) |
N1ii—Co1—N1 | 89.47 (6) | C2—Mn1—C2x | 90.20 (7) |
N1iii—Co1—N1 | 180.00 (10) | C2vii—Mn1—C2x | 90.20 (7) |
N1iv—Co1—N1 | 90.53 (6) | C2viii—Mn1—C2x | 180.00 (7) |
N1i—Co1—N1v | 90.53 (6) | C2ix—Mn1—C2x | 89.80 (7) |
N1ii—Co1—N1v | 89.47 (6) | Co1—N1—H1A | 109.5 |
N1iii—Co1—N1v | 90.53 (6) | Co1—N1—H1B | 109.5 |
N1iv—Co1—N1v | 180.00 (10) | H1A—N1—H1B | 109.5 |
N1—Co1—N1v | 89.47 (6) | Co1—N1—H1C | 109.5 |
C2vi—Mn1—C2 | 180 | H1A—N1—H1C | 109.5 |
C2vi—Mn1—C2vii | 90.20 (7) | H1B—N1—H1C | 109.5 |
C2—Mn1—C2vii | 89.80 (7) | N2—C2—Mn1 | 178.31 (17) |
C2vi—Mn1—C2viii | 90.20 (7) | | |
Symmetry codes: (i) y, −x+y, −z; (ii) −y, x−y, z; (iii) −x, −y, −z; (iv) x−y, x, −z; (v) −x+y, −x, z; (vi) −x+2/3, −y+4/3, −z+1/3; (vii) −y+1, x−y+1, z; (viii) −x+y, −x+1, z; (ix) y−1/3, −x+y+1/3, −z+1/3; (x) x−y+2/3, x+1/3, −z+1/3. |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···N2vii | 0.89 | 2.09 | 2.979 (2) | 173 |
Symmetry code: (vii) −y+1, x−y+1, z. |
Experimental details
Crystal data |
Chemical formula | [Co(NH3)6][Mn(CN)6] |
Mr | 372.19 |
Crystal system, space group | Trigonal, R3 |
Temperature (K) | 100 |
a, c (Å) | 10.963 (5), 10.779 (5) |
V (Å3) | 1121.9 (9) |
Z | 3 |
Radiation type | Mo Kα |
µ (mm−1) | 1.96 |
Crystal size (mm) | 0.35 × 0.26 × 0.25 |
|
Data collection |
Diffractometer | Bruker SMART APEXII CCD area-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Bruker, 2004) |
Tmin, Tmax | 0.546, 0.614 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 3602, 628, 497 |
Rint | 0.038 |
(sin θ/λ)max (Å−1) | 0.667 |
|
Refinement |
R[F2 > 2σ(F2)], wR(F2), S | 0.025, 0.071, 0.93 |
No. of reflections | 628 |
No. of parameters | 32 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.29, −0.43 |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···N2i | 0.89 | 2.09 | 2.979 (2) | 172.9 |
Symmetry code: (i) −y+1, x−y+1, z. |
Our interest is in the use of cyanometalates as molecular building blocks for potentially constructing clusters and networks with adjustable magnetic properties [Przychodzen et al., (2006), Withers et al., (2005)].
The title compound crystallizes in the trigonal R-3 space group with Z = 3. The main part of the asymmetric unit contains one Co and one Mn atom, both lying on threefold rotational axes.
The octahedral environments around CoII and MnII are generated by symmetry and shows very slight deviation from ideal geometry as illustrated by the C—Mn—C angles of 180.00 (7), 89.80 (7) and 90.20 (7) and N—Co—N angles of 180.00 (7), 89.47 (6) and 90.53 (6) ° respectively.
A three dimensional network is created by hydrogen bonds of the type N—H—N.