Startseite Complete X-ray single-crystal structure determination and Raman spectrum of NH4[C(CN)3]
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Complete X-ray single-crystal structure determination and Raman spectrum of NH4[C(CN)3]

  • Olaf Reckeweg EMAIL logo , Armin Schulz und Francis J. DiSalvo
Veröffentlicht/Copyright: 12. Juni 2017
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Abstract

The crystal structure of NH4[C(CN)3] has been determined via X-ray single-crystal methods at 203(2) K corroborating earlier results. Additionally, the hydrogen positions have been determined and the Raman spectrum of the title compound recorded on single crystals. The spectroscopic results are compared to those for related compounds.

1 Introduction

Ionic tricyanomethanides with the composition A[tcm] (A: Na, K or NH4; [tcm]≡[C(CN)3]) were obtained in the late 1950s of the last century by Trofimenko et al. [1] and structurally characterized soon after the initial preparation of the anion [2], [3], [4], [5]. Nevertheless, it took more than 50 years before the rubidium and the cesium compound were characterized [6], [7], and next to the still elusive crystal structure of Li[tcm], the crystal structure of NH4[tcm] [4] is still incomplete – the positions of the hydrogen atoms are still amiss and – as far as we know – no vibrational data are on record for this compound.

While pursuing research with tricyanomethanides, we synthesized some crystals of NH4[tcm], determined its complete crystal structure via single-crystal X-ray methods at 203 K and recorded its Raman spectrum on the same crystals used also in X-ray diffraction.

2 Experimental section

2.1 Synthesis

Ag[tcm] was synthesized by blending an aqueous solution containing 200 mg (2.25 mmol) K[tcm] (96%, powder, Alfa Aesar, Ward Hill, MA, USA) with a solution containing 400 mg (2.35 mmol) of AgNO3 (≥99%, Sigma-Aldrich, St. Louis, MO, USA). The off-white precipitate was washed with deionized water and dried using an aspirator. The precipitate was mixed with 50 mg (1.2 mmol) NH4Cl (≥99%, Sigma-Aldrich, St. Louis, MO, USA) in 5 mL of deionized water. After stirring this mixture for 6 h, the resulting solution was filtered to remove the precipitated AgCl. The water was evaporated in a drying oven at 80°C. The material crystallizes in form of plates and is not hygroscopic and appears to be stable over periods of several weeks.

2.2 Crystallographic studies

Samples of NH4[tcm] taken out of the drying oven were immersed in dried polybutene oil (Aldrich, St. Louis, MO, USA, M~320, isobutylene>90%) for single-crystal selection under a polarization microscope, mounted in a drop of polybutene sustained in a plastic loop, and placed onto the goniometer in a cold stream of nitrogen [T=203(2) K] which froze the polybutene oil, thus keeping the crystal stationary and protected from oxygen and moisture in the air. Intensity data were collected with a Bruker X8 Apex II diffractometer equipped with a 4 K CCD detector and graphite-monochromatized MoKα radiation (λ=71.073 pm). The intensity data were handled with the program package [8] that came with the diffractometer. The intensity data were corrected for Lorentz and polarization effects, but due to the low X-ray absorbance of NH4[tcm], no other absorption correction was applied. Systematic absences led to the space group P21/c. The program Shelxs-97 [9], [10] found the carbon and nitrogen positions with the help of Direct Methods. The hydrogen positions were apparent from the positions of the highest electron density on the difference Fourier map resulting from the first refinement cycle by full-matrix least-squares techniques with Shelxl-97 [11], [12]. Doing further refinement cycles, the refinement converged and resulted in a stable model for the crystal structure. Additional crystallographic details are described in Table 1. Atomic coordinates and equivalent isotropic displacement coefficients are shown in Table 2. Table 3 displays the anisotropic displacement parameters and Table 4 shows selected distances and angles.

Table 1:

Summary of single-crystal X-ray diffraction structure determination data of NH4[tcm].

CompoundNH4[C(CN)3]≡NH4[tcm]
Mr108.11
Crystal colorTransparent colorless
Crystal shapePlate
Crystal size, mm30.12×0.08×0.02
Crystal systemMonoclinic
Space group (no.)P21/c, (14)
Z4
Lattice parameters
a, pm908.1(2)
b, pm382.37(9)
c, pm1725.8(4)
β, deg104.915(10)
V, Å3579.1(2)
Dcalcd, g cm−31.24
F(000), e224
μ, mm−10.1
DiffractometerBruker X8 Apex II with a 4 K CCD
Radiation/λ, pm/monochromatorMoKα /71.073/graphite
T, K203(2)
Ranges, 2θmax, deg50.6
hkl range–10→9, ±4, ±20
Reflections: measured/unique4286/1048
Unique reflections with Fo >4σ (Fo )600
Rint/Rσ0.060/0.071
Refined parameters90
R1a/wR2b/GoFc (all refl.)0.097/0.109/0.941
Max. shift/esd, last refinement cycle<0.00005
Δρfin (max/min), e Å−30.15/–0.17
CSD number432839
  1. aR1=Σ ||Fo|–|Fc||/Σ |Fo|; bwR2=[Σw(Fo2Fc2)2/Σ(wFo2)2]1/2; w=1/[σ2(Fo2)+(xP)2+yP], where P=[(Fo2)+2Fc2]/3 and x and y are constants adjusted by the program; cGoF(S)=[Σw(Fo2Fc2)2/(np)]1/2, with n being the number of reflections and p being the number of refined parameters.

Table 2:

Atomic coordinates and equivalent isotropic displacement parametersa of NH4[tcm].

AtomxyzU11U22U33U23U13U12Ueq
NH14e0.6721(3)0.0303(6)0.5925(1)198(13)166(12)164(12)18(10)24(9)–2(11)180(5)
H14e0.685(3)0.138(7)0.632(1)402(82)b
H24e0.598(3)0.893(7)0.588(1)402(82)b
H34e0.653(3)0.141(7)0.556(1)402(82)b
H44e0.746(3)0.906(7)0.594(1)402(82)b
C04e0.2018(3)0.3445(6)0.6391(1)306(14)313(15)287(13)17(10)109(11)–4(11)296(6)
C14e0.3073(3)0.4588(6)0.5985(1)315(14)306(16)295(13)12(11)34(12)5(11)313(6)
C24e0.0496(3)0.4586(6)0.6149(1)381(17)341(16)337(14)–15(11)140(12)–48(13)344(7)
C34e0.2527(3)0.1612(6)0.7123(1)377(15)294(15)360(14)–62(13)120(12)–6(12)339(7)
N14e0.3923(2)0.5543(5)0.5638(1)340(13)495(16)386(12)79(10)133(10)30(11)400(6)
N24e0.9253(3)0.5556(6)0.5954(1)351(14)549(17)537(14)57(11)138(11)32(12)475(7)
N34e0.2932(2)0.0136(6)0.7723(1)604(16)414(15)362(12)27(11)112(11)–15(12)462(7)
  1. aUeq is defined as a third of the orthogonalized Uij tensors; bthe isotropic displacement factor of the hydrogen atom was constrained to the equivalent displacement factor of NH1 as the last unconstrained atom as suggested in Ref. [11].

Table 3:

Selected bond lengths (pm) and angles (deg) of NH4[tcm].

NH1–H178(2)C0–C1139.5(3)
H284(2)C2140.6(4)
H374(2)C3141.4(3)
H482(2)C1–N1115.8(3)
H1N3215(2)C2–N2115.4(3)
H2N1221(2)C3–N3115.4(3)
H3N1232(2)
H4N2211(2)
∡(C0–C1–N1)179.1(2)∡(C1–C0–C2)120.2(2)
∡(C0–C2–N2)179.3(3)∡(C1–C0–C3)119.7(2)
∡(C0–C3–N3)179.3(3)∡(C2–C0–C3)119.3(2)
Table 4:

Raman spectra of NH4[tcm], K[tcm] [13], Rb[tcm] [7] and Cs[tcm] [7].a

NH4[tcm]K[tcm] [13]Rb[tcm] [7]Cs[tcm] [7]
Lattice vibrations47/72/84

102/175/203
101/19389/194
δ(C–C3 i.p.)480 w483 w490 vw484 vw
δ(C–C≡N i.p.)572 w609 vw
ν(C–C)667 m657 vw649 m648 m
δ(C–C), only for C3h960/981 vw973 w974 vw972 vw
ν(C–C)1245 w1243 s1239 vw1232 vw
ν(C–C)1266 vw1267 vw1265 vw
δ(NH4+)1440 w
ν(C≡N)2170 m2134 vw2129 vw
ν(C≡N)2186 s/2231 vs2175/2225 vs2178/2222 vs2175/2220 vs
ν(NH4+)2854 w/3041 w

3101 w/3168 w
  1. aw, weak; m, medium; s, strong; v, very; i.p., in plane.

Further details of the crystal structure investigation may be obtained from FIZ Karlsruhe, 76344 Eggenstein-Leopoldshafen, Germany (fax: +49-7247-808-666; e-mail: ) on quoting the deposition number CSD-432839 for NH4[tcm].

2.3 Raman spectroscopy

Transparent colorless single crystals of NH4[tcm] sealed in thin-walled glass capillaries were used for the Raman-spectroscopic investigations, which were performed on a microscope laser Raman spectrometer (Jobin Yvon, Unterhaching, Germany), 4 mW, equipped with a HeNe laser with an excitation line at λ=632.817 nm, 50× magnification, and 8×240 s accumulation time. The Raman spectrum is displayed in Fig. 1 and the vibrational data are shown together with those of related compounds [7], [13] in Table 4.

Fig. 1: Raman spectrum of NH4[tcm]. Both insets are enlarged by the factor of 25 on the vertical axis.
Fig. 1:

Raman spectrum of NH4[tcm]. Both insets are enlarged by the factor of 25 on the vertical axis.

3 Results and discussion

3.1 Raman spectrum

The Raman spectrum of the title compound shows frequencies indicating unambiguously the presence of the ammonium and tricyanomethanide ions (Table 4). Weak bands indicating the presence of the NH4+ cation are observed in the expected region around 2800–3400 cm−1. Modes with very weak intensities around 959 cm−1 and 980 cm−1 are observed for the anion which is predicted to be Raman-active only for C3h symmetry [13]. Anyhow, the observed intensities of these modes might be seen as indication, but not as proof for a deviation of the anion from the ideal D3h symmetry (see paragraph ‘Crystal structure’).

3.2 Crystal structure of NH4[tcm]

The four hydrogen atoms of the cation exhibit N–H bond lengths around 80 pm. This is shorter than expected, but this is likely an artifact of the structure determination method using X-rays for locating electron densities. All four H atoms are located near a direct line drawn from the central nitrogen atom of NH4+ to the closest nitrogen atom belonging to different [tcm] anions. These N–N distances are all near 300 pm. Within a distance below 350 pm, four more N–N contacts complete the coordination sphere of the ammonium cation in NH4[tcm] forming a distorted cube (Fig. 2, left; Table 3).

Fig. 2: Coordination of the ammonium cation (left) and the tricyanomethanide anion (right). Thick black lines indicate covalent bonding, the thin lines indicate hydrogen bonds towards nitrogen.
Fig. 2:

Coordination of the ammonium cation (left) and the tricyanomethanide anion (right). Thick black lines indicate covalent bonding, the thin lines indicate hydrogen bonds towards nitrogen.

The [tcm] anion is surrounded by four ammonium ions, in which N1 is coordinated by two cations, and each N2 and N3 by one cation. The [tcm] moiety is slightly distorted by this unsymmetric coordination, but equivalent bonds have the same bond length within three times the standard deviations (Fig. 2, right; Table 3). The central C0 atom is slightly out of the plane defined by N1, N2 and N3 by a little less than 0.15 pm, but this is not more than one standard deviation of any bond length determined in this work.

NH4+ and [tcm] ions are stacked above each other along the crystallographic b axis (Fig. 3). These stacks of NH4+ and [tcm] ions alternate along the crystallographic a axis forming layers. Double layers form parallel to the (ab) plane in which the [tcm] ions of each monolayer are tilted about 30° due to the 21/c screw axis symmetry with respect to the crystallographic c axis (Fig. 4) to achieve maximal packing density within the double layers.

Fig. 3: Perspective view of the unit cell of NH4[tcm] along to the crystallographic b axis. Thick black lines indicate covalent bonding, the thin lines indicate hydrogen bonds towards nitrogen.
Fig. 3:

Perspective view of the unit cell of NH4[tcm] along to the crystallographic b axis. Thick black lines indicate covalent bonding, the thin lines indicate hydrogen bonds towards nitrogen.

Fig. 4: Non-perspective view perpendicular to the (bc) plane. Thick black lines indicate covalent bonding, the thin lines indicate hydrogen bonds towards nitrogen.
Fig. 4:

Non-perspective view perpendicular to the (bc) plane. Thick black lines indicate covalent bonding, the thin lines indicate hydrogen bonds towards nitrogen.

4 Conclusion

The structure of NH4[tcm] has been determined more precisely than before including the hydrogen atoms of the NH4+ ion corroborating and complementing the structural data reported before [4]. To the best of our knowledge, the Raman spectrum of the title compound was recorded for the first time. On the basis of our structural and spectroscopic data, no valid distinction between the C3h and the ideal D3h symmetry of the [tcm] anion can be stated.

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Received: 2017-3-30
Accepted: 2017-4-21
Published Online: 2017-6-12
Published in Print: 2017-6-27

©2017 Walter de Gruyter GmbH, Berlin/Boston

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