Open Access Article
Bingjia
Yan‡
,
Peter N.
Horton
,
Simon C.
Weston§
,
Andrea E.
Russell
and
Martin C.
Grossel
*
School of Chemistry, University of Southampton, Highfield, Southampton, SO17 1BJ, UK. E-mail: M.C.Grossel@soton.ac.uk; Fax: +44 (0)23 8059 3781; Tel: +44 (0)23 8059 3153
First published on 31st August 2021
An investigation of the solid-state behaviour of five 12-crown-4 alkali metal TCNQ complexes, (12-crown-4)2LiTCNQ (1), (12-crown-4)2NaTCNQ (2), (12-crown-4)2Li(TCNQ)2 (3), (12-crown-4)2Na(TCNQ)2 (4), and (12-crown-4)2K(TCNQ)2 (5), reveals an unusual “cross-stitch” packing motif with the extended face-to-face π-stacked TCNQ˙− columns present in complexes 1 and 2. The effect of the presence of additional neutral TCNQ0 has also been explored.
We have previously reported detailed studies of the solid-state behaviour of a range of ionophore-complexed alkali metal–TCNQ˙− salts including 15-crown-5 and 18-crown-6 complexes of Li+, Na+, K+, Tl+ and Rb+TCNQ˙−1,17,19,22–25 and 15-crown-5 complexes of Li+ and Na+ (TCNQ˙−)(TCNQ0).25 Recently, Akutagawa and co-workers26,27 have reported the crystal structure of Li+(12-crown-4)2(TCNQ)2 and Na+(12-crown-4)2(TCNQ)2, but there is limited information to the solid-state behaviour of other 12-crown-4 alkali metal TCNQ complexes.
In this paper, we report the synthesis and crystallographic studies of five 12-crown-4 alkali metal TCNQ complexes, two simple TCNQ salts: (12-crown-4)2LiTCNQ (1), and (12-crown-4)2NaTCNQ (2); and three related complex TCNQ salts: (12-crown-4)2Li(TCNQ)2 (3), (12-crown-4)2Na(TCNQ)2 (4), and (12-crown-4)2K(TCNQ)2 (5) (see Scheme 1).
–
stretch), 2173, 2151 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[triple bond, length as m-dash]](https://www.rsc.org/images/entities/char_e002.gif)
stretch), 1589 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
(CN)2 stretch), 1505 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
ring stretch), 1361 (
–
bend), 1177 (
–
N and
–
ring stretch), 986 (C–C ring stretch), 819, 718 (
–
out of plane bend). Raman vmax/cm−1 2214 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[triple bond, length as m-dash]](https://www.rsc.org/images/entities/char_e002.gif)
stretch), 1604 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
ring stretch), 1384 (
–
N stretch), 1208 (C![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
–
bending). M.p. 234 °C (dec.). Elemental analysis: calculated: C: 59.68%, H: 6.44%, N: 9.94%. Found: C: 59.80%, H: 6.15%, N: 10.36%.
–
stretch), 2172, 2150 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[triple bond, length as m-dash]](https://www.rsc.org/images/entities/char_e002.gif)
stretch) (lit.34 2177, 2156), 1567 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
(CN)2 stretch), 1505 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
ring stretch), 1361 (
–
bend), 1177 (
–
N and
–
ring stretch), 986 (C–C ring stretch), 820, 718 (
–
out of plane bend). Raman vmax/cm−1 2257 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[triple bond, length as m-dash]](https://www.rsc.org/images/entities/char_e002.gif)
stretch), 1609 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
ring stretch), 1389 (
–
N stretch), 1206 (C![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
–
bending). M.p. 226 °C (dec.) (lit.34 185–187 °C). Elemental analysis: calculated: C: 58.03%, H: 6.22%, N: 9.67%. Found: C: 57.64%, H: 6.16%, N: 9.48%.
–
stretch), 2215, 2188 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[triple bond, length as m-dash]](https://www.rsc.org/images/entities/char_e002.gif)
stretch), 1558 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
(CN)2 stretch), 1507 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
ring stretch), 1327 (
–
bend), 1134 (
–
N and
–
ring stretch), 953 (C–C ring stretch), 861, 694 (
–
out of plane bend). Raman vmax/cm−1 2216 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[triple bond, length as m-dash]](https://www.rsc.org/images/entities/char_e002.gif)
stretch), 1606 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
ring stretch), 1385 (
–
N stretch), 1207 (C![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
–
bending). M.p. 312 °C (dec.).
–
stretch), 2223, 2201, 2177 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[triple bond, length as m-dash]](https://www.rsc.org/images/entities/char_e002.gif)
stretch), 1560 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
(CN)2 stretch), 1506 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
ring stretch), 1302 (
–
bend), 1136 (
–
N and
–
ring stretch), 951 (C–C ring stretch), 848, 689 (
–
out of plane bend). Raman vmax/cm−1 2212 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[triple bond, length as m-dash]](https://www.rsc.org/images/entities/char_e002.gif)
stretch), 1602 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
ring stretch), 1382 (
–
N stretch), 1206 (C![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
–
bending). M.p. 310 °C (dec.)
–
stretch), 2195, 2179, 2167 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[triple bond, length as m-dash]](https://www.rsc.org/images/entities/char_e002.gif)
stretch), 1560 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
(CN)2 stretch), 1508 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
ring stretch), 1363 (
–
bend), 1181 (
–
N and
–
ring stretch), 956 (C–C ring stretch), 828, 700 (
–
out of plane bend). Raman vmax/cm−1 2217 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[triple bond, length as m-dash]](https://www.rsc.org/images/entities/char_e002.gif)
stretch), 1608 (![[C with combining low line]](https://www.rsc.org/images/entities/char_0043_0332.gif)
![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
ring stretch), 1390 (
–
N stretch), 1204 (C![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif)
–
bending). M.p. >300 °C (dec.). Elemental analysis: calculated: C: 60.06%, H: 5.04%, N: 14.00%. Found: C: 59.82%, H: 4.44%, N: 15.74%.
For (12-crown-4)2LiTCNQ (1) and (12-crown-4)2NaTCNQ (2), some difficulties were encountered during the X-ray crystal structure solution as the 12-crown-4 moieties are disordered. The atomic occupancy of the disordered 12-crown-4 units in 1 is 0.504(2): 0.496(2) and 0.5: 0.5 in 2, respectively. Complexes 1 and 2 are iso-structural. In each case, the alkali metal cation (Li+ and Na+) is sandwiched between two 12-crown-4 units and is thus completely screened from the TCNQ˙− counter anion (see Fig. 1). This situation is similar to that seen previously for the (15-crown-5)2KTCNQ (6),1 in which one K+ cation is sandwiched between two disordered 15-crown-5 ether ligands at room temperature, the presence of the ionophore sandwich preventing direct cation–anion contacts.1
![]() | ||
| Fig. 1 Unit cell of TCNQ complexes (a). (12-crown-4)2LiTCNQ (1) and (b). (12-crown-4)2NaTCNQ (2). In each case, the 12-crown-4 ether ligands are disordered. | ||
The TCNQ˙− anions are face-to-face π-stacked in both 1 and 2 (see Fig. 2), in which neighbouring anion planes are tilted in respect to each other (6.27° in 1 and 6.89° in 2) forming a novel “cross-stitch”-like stack (see Fig. 2a and c). A top view of adjacent TCNQ˙− units reveals that neighbouring TCNQ˙− anions are significantly long-axis slipped and slightly short-axis slipped (see Table 1 and Fig. 3 for the key structural details). Furthermore, adjacent TCNQ˙− anions are mutually twisted in respect to each other (26.02° in 1 and 26.00° in 2) (see Fig. 2b and d). To our knowledge, this “cross-stitch”-like twisted packing motif of neighbouring TCNQ˙− units is a novel packing motif for alkali metal TCNQ complexes.
![]() | ||
| Fig. 2 Side (a) and top (b) views of the TCNQ˙− dimer in (12-crown-4)2LiTCNQ (1) in respect to the views (c and d) of (12-crown-4)2NaTCNQ (2). | ||
| Complex | π–π separation/Å | Long-axis slippage/Å | Short-axis slippage/Å | Ref. |
|---|---|---|---|---|
| 1. (at 100 K) | — | 2.40 | 0.26 | This work |
| 2. (at 100 K) | — | 2.34 | 0.23 | This work |
| 3. (at 100 K) | 3.153 | 1.99 | 0.48 | This work |
| 4. (at 100 K) | 3.123 | 2.04 | 0.33 | This work |
| 5. (at 100 K) | 3.125 | 2.03 | 0.30 | This work |
![]() | ||
| Fig. 3 Definition of short and long-axis slippage (a), twist angle φ (b), and tilt angle δ (c) in this study (see Table 1). | ||
In the solid state, both 1 and 2 the TCNQ˙− moiety and the cation-crown ether complex (12-crown-4)2M+ (M+ = Li+ and Na+) form mixed 1
:
2 alternating sheets, in a manner similar to that previously reported for 61 (see Fig. 4a and b).
![]() | ||
| Fig. 4 A top view of the solid-state structure of (12-crown-4)2LiTCNQ (1, a) and (12-crown-4)2NaTCNQ (2, b). | ||
Viewed from the side, both the TCNQ˙− dimers and the cation barrels formed by the (12-crown-4)2M+ (M+ = Li+ and Na+) moieties in 1 and 2 are assembled further into infinite extended columns (see Fig. 5). The centroid–centroid distance between adjacent TCNQ˙− units within the column is 4.155 Å in 1 and 4.154 Å in 2. This packing motif in both 1 and 2 is clearly different from that seen for 6. In the latter case, TCNQ˙− anion dimers are isolated from each other, being surrounded by (15-crown-5)2K+ cation barrels.1
![]() | ||
| Fig. 5 Comparison of the side and top views of the extended columns formed by (12-crown-4)2LiTCNQ (1), (a) and (b) respectively, and by (12-crown-4)2NaTCNQ (2) (c) and (d) respectively. | ||
In the solid-state, the alkali metal cation (Li+, Na+, or K+) in each of the complex TCNQ salts (3–5) is coordinated to and sandwiched between two 12-crown-4 units. The resulting cation “barrels” of (12-crown-4)2M+ (M+ = Li+, Na+, and K+) inhibit any direct interaction between alkali metal cations and the TCNQ units (M+–NC), with the cation complexes sitting in channels between the infinite columns of face-to-face π-stacked (TCNQ)2˙− moieties (see Fig. 6 for example).
In 3–5, neighbouring (TCNQ)2˙− units form extended face-to-face π-stacked columns. Within the (TCNQ)2˙− units, the TCNQ moieties are significantly long-axis slipped (see Table 1 and Fig. 3 for the key structural details) with a vertical π–π separation of 3.153 Å in 3, 3.123 Å in 4, and 3.125 Å in 5, respectively. Additionally, individual TCNQ units adopt a shallow boat conformation, as previously reported by Akutagawa for Na+([12]-crown-4)2(TCNQ)2 at 100 K26 (see Fig. 7).
![]() | ||
| Fig. 7 Side and top views of the (TCNQ)2˙− dimer formed in (12-crown-4)2Na(TCNQ)2 (4) (a and b) and in (12-crown-4)2K(TCNQ)2 (5) (c and d). | ||
Furthermore, in 3–5, two pairs of TCNQ dimer units assemble into extended tetramers forming parallel sheets, which are separated by the corresponding cation barrels of (12-crown-4)2M+ (M+ = Li+, Na+, and K+) (see Fig. 8). This observation of tetramer packing motif is consistent with that reported by Akutagawa and co-workers for Li+([12]-crown4)2(TCNQ)2, and Na+([12]-crown4)2(TCNQ)2, in which two kinds of TCNQ units (A and B) form (A⋯B) face-to-face π-stacked dimers at 100 K with additional interdimer interactions ⋯(A⋯B)⋯(B′⋯A')⋯.26,27Fig. 8 illustrates this behaviour for 3 (please refer to ESI† (Fig. S1 and S2) for the corresponding information in 4 and 5.).
![]() | ||
| Fig. 8 Side (a) and top (b) views of the sheets of face-to-face π-stacked columns of TCNQ dimers formed in (12-crown-4)2Li(TCNQ)2 (3), revealing the long-axis slipped character of the TCNQ dimer. | ||
This repetitive pattern of tetramers further assembles into infinite TCNQ columns (see Fig. 9). The similarity of the bond lengths within the TCNQ columns makes it difficult to distinguish between the TCNQ˙− and neutral TCNQ0 components [please refer to ESI† (Fig. S3 and S4) for the corresponding figures for 4 and 5.].
![]() | ||
| Fig. 9 Side (a) and top (b) views of the packing motif of the alternating infinite columns of TCNQ units and cation barrels in (12-crown-4)2Li(TCNQ)2 (3). | ||
N stretches characteristic of the TCNQ˙− anion in 1 and 2. An extra band (at ∼2200 cm−1) indicates the presence of neutral TCNQ0 in 3–5. In the spectra, the C
C and C
N stretching bands of TCNQ units will generate obvious Raman peaks because the π electrons are strongly polarisable.37 For the TCNQ complexes (1–5), the peaks in the region 2217 and 2206 cm−1 are ascribed to stretching bands for cyano groups in TCNQ molecule.37 The peak between 1390 and 1380 cm−1 reflects electron transfer between neutral TCNQ0 and TCNQ˙−.37,38
| Compound | Infrared data/cm−1 | Raman data/cm−1 | Ref. | |||
|---|---|---|---|---|---|---|
C N stretch |
C C stretch |
C N stretch |
C C stretch |
C–C N stretch |
||
| TCNQ0 | 2228, 2225 | 1545 | 2225 | 1600 | 1450 | 36 |
| TCNQ0 | 2224, 2220 | 1545 | 2230 | 1603 | 1454 | This work |
| LiTCNQ | 2201, 2171 | 1501 | This work | |||
| NaTCNQ | 2197, 2184, 2160 | 1505 | 2204 | 1602 | 1384 | This work |
| KTCNQ | 2215, 2152 | 1505 | This work | |||
| 1 | 2173, 2151 | 1505 | 2214 | 1604 | 1384 | This work |
| 2 | 2172, 2150 | 1505 | 2206 | 1609 | 1389 | This work |
| 3 | 2222, 2198, 2165 | 1507 | 2216 | 1606 | 1385 | This work |
| 4 | 2223, 2201, 2177 | 1506 | 2212 | 1602 | 1382 | This work |
| 5 | 2195, 2179, 2167 | 1508 | 2217 | 1608 | 1390 | This work |
Footnotes |
| † Electronic supplementary information (ESI) available: Including additional figures and key crystallographic information. CCDC 2101940–2101944. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/d1ce01075a |
| ‡ Current address: Leibniz-Forschungsinstitut für Molekulare Pharmakologie, 13125 Berlin, Germany. |
| § Current address: Corporate Strategic Research, ExxonMobil Research & Engineering Company, Annandale, NJ 08801, USA. |
| This journal is © The Royal Society of Chemistry 2021 |