Solvent-dependent valence tautomerism and polarization switching in a heterodinuclear [CrCo] complex (2024)

Wenwei Zheng, Xiaopeng Zhang, Qirui Shui, Tatsuki f*ckuyama, Wen-huang Xu, Yu-bo Huang, Tianchi Ji, Ziqi Zhou, Mikoto Uematsu, Sheng-Qun Su, Shinji Kanegawa, Shu-Qi Wu* and Osamu Sato*
Institute for Materials Chemistry and Engineering & IRCCS, Kyushu University, 744 Motooka, Nishi-ku, f*ckuoka 819-0395, Japan. E-mail: sato@cm.kyushu-u.ac.jp

Received 2nd April 2024, Accepted 11th May 2024

First published on 17th May 2024

Introduction

Polar materials responsive to external stimuli, such as temperature, light, and electric field, offer potential applications in next-generation molecular memory devices.1–7 Ferroelectric materials where spontaneous polarization could be reversed by the application of an electric field have been the most intensively investigated polarization-switching materials. However, as a collective phenomenon in its nature, the rational design of ferroelectrics with the desired performance usually represents a formidable challenge from a chemical perspective.8–12 To diversify polarization-switching materials, a bottom-up approach, utilizing dynamic molecules with switchability between states and different electric dipole moments, has been proposed for non-ferroelectric systems to realize polarization switching. In this regard, valence tautomeric (VT) molecules are ideal structural motifs exhibiting variable electronic configurations responsive to temperature, pressure, and external fields.13–48 Furthermore, for crystalline materials with switchable macroscopic polarization, it is imperative that the target molecules crystallize in polar space groups so that their dipole moments will not be canceled. To date, there have been only a few non-ferroelectric molecular crystals exhibiting macroscopic polarization switching via electron transfer owing to the difficulties in crystal engineering to align molecules in polar space groups.14,18,49–51 The acquisition of such crystals still largely relies on serendipity. Hence, it is still full of challenges in synthesizing polar crystals through an appropriate molecular design to enhance the probability of arranging target molecules in a polar space group.

Recently, a series of dinuclear VT complexes with racemic ligands in a polar space group were synthesized via a chiral-assisted approach, which relies on the preference of left-handed chiral ligands to interact with their right-handed counterparts, resulting in a polar crystal structure.3,5,46,47 A natural extension would be the introduction of enantiopure ligands to enhance the possibility of obtaining polar crystals. Indeed, subsequent research in the case of mononuclear cobalt complexes has demonstrated its efficacy in diversifying polar crystals with VT behavior.2,40,52 However, the previously used crystallization strategy is invalid for dinuclear systems with hom*ochiral ligands due to the lack of complementary interactions. Therefore, the [Co^IICo^III] complex with an enantiopure SS-cth ligand was first investigated (cth = (7S,14S)-5,5,7,12,12,14-hexamethyl-1,4,8,11-tetraazacyclotetradecane) to aid in our initial screening. Although it is in the high-spin (HS) state in the temperature range between 2 and 400 K, the complex indeed crystallizes in the polar P2₁ space group with a regular molecular arrangement, where the Co^II sites are well distinguished from the Co^III sites crystallographically. This is a crucial factor for dictating directional electron transfer aiming at polarization-switching behavior. Given the fact that the strong coupling between chromium and dhbq proves beneficial for stabilizing a low-spin trivalent cobalt state,53 thereby enhancing the VT transition temperature in the corresponding racemic system, a site-selective substitution with Cr^III ions for Co^III sites would possibly lead to the desired VT behavior. Consequently, we synthesized the [CrCo] complex with the enantiopure SS-cth ligand. By careful design of synthetic procedures by first incorporating the more inert Cr³⁺ sites, we successfully isolated and obtained the pure heterometallic dinuclear [CrCo] complex [Cr(SS-cth)(μ-dhbq)Co(SS-cth)](PF₆)₃·2.5H₂O·0.5MeOH ((denoted as compound 1·sol), H₂dhbq = 2,5-dihydroxy-1,4-benzoquinone). Single-crystal structural analysis revealed that 1·sol is isostructural to the above-mentioned [Co^IICo^III] complex. Magnetometry and spectroscopic studies showed that 1·sol exhibits an incomplete VT transition between the Co ion and the dhbq ligand. Polarization switching from such an intramolecular electron transfer process could be directly probed by pyroelectric measurements. Upon heating, the crystals still retain their integrity without changing the space group. Interestingly, detailed structural analysis and magnetometry revealed that the desolvated complex, 1, exhibits a much more complete VT behavior. When exposed to water–methanol vapor, complex 1 can re-absorb the solvent molecules, recovering to its solvated form, 1·sol, with incomplete VT. Such solvent-induced switching of physical behavior could be repeatedly observed.

Results and discussion

Three heterometallic dinuclear complexes [MCr] (M = Co, Zn, Ni) featuring the enantiopure ligand SS-cth or RR-cth were synthesized according to one-pot and stepwise routes. In the former, enantiomeric complexes ([M(AcO)(SS-cth)]PF₆ and [CrCl₂(SS-cth)]Cl) were obtained separately and mixed in a methanol solution of dhbq, resulting in a crude complex [Cr(SS-cth)(μ-dhbq)(M(SS-cth))](PF₆)₃. In the latter, the [Cr(SS-cth)(μ-dhbq)]PF₆ precursor was first isolated and then mixed with the corresponding complex motif to afford heterometallic [CrM] complexes, exemplified by [CrCo] (Fig. 1). The characterization of complexes using mass spectra confirmed that the stepwise method effectively yields pure heterometallic complexes. The crude samples obtained from the two methods were dissolved in MeOH and mass spectral measurements were subsequently conducted. By the one-pot route, the obtained spectrum shows three distinct types of molecular peaks for [1(PF₆)₂]⁺ (m/z = 1107.9) through conventional methods, including [(CrCr)(PF₆)₂]⁺, [(CrCo)(PF₆)₂]⁺, and [(CoCo)(PF₆)₂]⁺. Notably, alongside the predominant [CrCo] peaks, the intensity of peaks attributed to [CoCo] is remarkably strong, indicating a discernible random occupation of the two coordination sites during synthesis (Fig. 2a). In contrast, the spectrum of [1(PF₆)₂]⁺ obtained using the stepwise method reveals nearly all molecular peaks contributed by [CrCo] (Fig. 2b), consistent with calculated results (Fig. S1†). Moreover, the mass spectra of reference complexes, [NiCr] and [ZnCr], also validate the universality of the stepwise synthetic route (Fig. S2 and S3†). These findings strongly support the feasibility of the new strategy for synthesizing pure heterometallic complexes with an enantiopure ligand.

Temperature-dependent single-crystal X-ray diffraction of 1·sol and 1 was performed at 100, 150, 200, and 375 K. The structural analyses revealed that both 1·sol and 1 crystallize in the polar P2₁ space group throughout the studied temperature range. The asymmetric unit of 1·sol involves one heterodinuclear molecular ion comprising [Co(SS-cth)] and [Cr(SS-cth)] motifs bridged by a dhbq ligand, three PF₆⁻ anions, two and a half water molecules, and a half-occupied methanol molecule. The composition of the co-crystallized solvent is further supported by thermogravimetric analysis (TGA) and elemental analysis (Fig. S4†). Interestingly, different from the eclipsed conformation in the previously reported heterochiral [CrCo] complex, the two SS-cth ligands in the complex motif of 1·sol adopted a slightly staggered conformation. Such a structural distortion may contribute to different VT transition behavior. At 100 K, 1·sol exhibited the average Co–O and Co–N bond lengths of 2.069 and 2.149 Å, indicative of the dominant presence of the Co²⁺ HS ions, while the average bond lengths of Cr–O and Cr–N bonds are 1.940 and 2.086 Å, characteristic of the Cr³⁺ ions. The evident differences in metal–ligand bond lengths clearly show that the Co and Cr sites are well distinguished rather than a random occupation. By the 2₁-screw rotation, the [CrCo] molecular motif is regularly packed, with a uniform projection angle (70.31(7)°) along the crystallographic b-axis, a critical factor for the manifestation of polarization switching (Fig. 3, upper). Upon heating above room temperature, the sample started to diffract badly until 375 K, where all the solvent molecules were removed according to the TGA result. Crystal structural analysis also confirmed the absence of solvent molecules in the lattice; thus, the diffraction data correspond to its desolvated form, 1. Notably, the bond lengths around the Co ions remained consistent with those typical for Co²⁺ ions. However, when the temperature was reduced back to 100 K, a significant contraction in cell volume by 184 ų was observed. Simultaneously, the average bond lengths around the Co ions contracted to 1.910 Å and 2.041 Å for Co–O and Co–N bonds, respectively, indicative of Co³⁺ LS ions. Furthermore, the observed contraction in the specific C–C bonds (C2–C3; C5–C6), accompanied by the elongation in the C–O bonds located on both sides of the bridging ligand, further confirms the occurrence of dhsq³⁻ in a low-temperature range after desolvation (Fig. S5a–c†). These significant changes in bond lengths at the Co site clearly indicate a more pronounced VT behavior in complex 1, transitioning to [Cr³⁺-dhsq³⁻-Co³⁺_LS] upon cooling. Additionally, the projection angle between the [CrCo] direction and the polar b-axis also alters to 85.66(1)° at 375 K and 85.35(8)° at 100 K after desolvation (Fig. 3, lower; S6†). Comparing the extent of VT transition and the changes in molecular arrangements before and after desolvation, we anticipate a solvent-tuned polarization change at the single-crystal level.

The variable-temperature powder X-ray diffraction (PXRD) technique was employed to confirm the reversibility of the crystal structure during the in situ desolvation–reabsorption process (Fig. 4). To prevent the escape of the removed solvent molecules, the powder sample of 1·sol was carefully sealed using aluminum foil, and measurements were performed by following the sequence of 230–400–230 K. The PXRD patterns of 1·sol at 230 K matched well with the simulated one from single-crystal data. No obvious change in these reflections was observed until the temperature reached 326 K. When the temperature was increased further to 376 K, the PXRD patterns showed a significant and complete change of reflections at 2θ = 10.0°, 11.4°, 12.3°, and 20.5°. This change was consistent with the calculated result of the desolvated complex 1 at 375 K, indicating that compound 1 was generated in situ. The powder patterns remained unchanged until 400 K. However, when cooled down again, the diffraction pattern did not match the simulated result of compound 1 at low temperature but reverted to that of the pristine compound, 1·sol. These results clearly certify that the desolvated crystal could reabsorb the trapped solvent under ambient conditions to recover to the solvated compound, 1·sol. We also performed the PXRD measurement on thermally treated compound 1. After exposure to MeOH and H₂O, the diffraction pattern agreed well with that of 1·sol (Fig. S7†). This also supported the reversibility of single-crystal-to-single-crystal transformation (SCSCT).54

Variable-temperature magnetic susceptibility was measured on the polycrystalline sample of 1·sol. To prevent the loss of co-crystallized solvent molecules, the measurements started from 260 K under a 2 kOe magnetic field with a cooling rate of 2 K min⁻¹ (Fig. 5). For compound 1·sol, the χ_mT value almost remains at 4.3 cm³ K cm⁻¹ from 260 to 220 K, which is in good agreement with the expected value of isolated metal centers on Cr³⁺ (S = 3/2) and high spin Co²⁺ (S = 3/2) with an unquenched orbital magnetic moment. Upon further cooling, a gradual decrease in the χ_mT value is observed, reaching a plateau at 3.7 cm³ K cm⁻¹ from 75 to 30 K. The VT transition temperature, defined as the peak temperature of the temperature derivative of the χ_mT plot, is determined to be ca. 170 K. On reheating to 260 K, the χ_mT value undergoes a reversible change without significant hysteresis. To explore the origin of this behavior, variable-temperature spectroscopic analyses were performed in the heating mode in this temperature range. A gradual decline in the intensity of the absorption band centered at 500 nm is observed, which is attributed to ligand–metal charge transfer from dhsq³⁻ to Co³⁺ ions (Fig. S8a†). Correspondingly, the vibrational band of dhsq³⁻ at 1470 cm⁻¹ also shows a remarkable decrease in the same temperature range (Fig. S8b†). These findings strongly indicate that the variation in the χ_mT values within this temperature range is associated with the partial electron transfer from the [Cr³⁺-dhsq³⁻-Co³⁺_LS] to the [Cr³⁺-dhbq²⁻-Co²⁺_HS] state. Upon further heating to 400 K, the χ_mT value reaches ca. 4.2 cm³ K cm⁻¹ accompanied by desolvation. The desolvated sample, 1, exhibits a more pronounced change. Below 340 K, the χ_mT value decreased abruptly and reached the minima 1.26 cm³ K cm⁻¹, corresponding to an almost complete transition to the [Cr³⁺-dhsq³⁻-Co³⁺_LS] state (expected χ_mT value: 1.0 cm³ K cm⁻¹). The transition temperature is estimated to be 215 K with no obvious hysteretic behavior. Similar changes could also be observed from UV-vis and IR absorption spectra. The ground powder sample adhered to a CaF₂ plate (for IR) and transparent tape (for UV-vis) was heated up to 400 K. After removal of the co-crystallized solvent molecules, the samples were quickly sealed into a vacuum tube to prevent the re-absorption of water molecules from air. The spectra of 1 were recorded from 79 to 300 K. At low temperature, two strong absorption peaks were observed at around 1210 and 1470 cm⁻¹, attributed to the C–O stretching vibration from dhsq³⁻. As the temperature increased, a continuous decay of these absorption peaks was observed, whereas the characteristic absorption peaks (approximately 1560 and 1270 cm⁻¹) belonging to dhbq²⁻ became more intense (Fig. S8c†). These results directly supported that a variation of the electronic structure occurred on the bridging ligand. The UV-vis spectra also revealed similar changes to those for the pristine compound, 1·sol, with different transition temperature domains (Fig. S8d†). Notably, when the absorption intensities of the characteristic absorption bands in IR and UV-vis spectra were plotted against temperature, a clear shift in the transition temperature range could be identified, in good agreement with the magnetic data of the solvent effect of this compound (Fig. S9a–c†).

Additionally, the desolvated powder sample was placed above a MeOH/H₂O mixture, ensuring no direct contact, and left overnight. Subsequently, the magnetic properties of the solvent-reabsorbed sample were measured under the same conditions as those for the original sample to confirm the recovery of magnetic properties upon solvent reabsorption. The results showed similar behavior, i.e., a partial and nearly complete electron transfer before and after solvent removal (Fig. S10†). Elemental analysis further corroborated the transition from compound 1 to 1·sol (Table S1†). These findings indicate that the solvent influence on the VT process of compound 1·sol can be reversibly manipulated through solvent reabsorption. Moreover, both compounds 1·sol and 1 exhibited more pronounced photoinduced valence tautomerism than the previous [CrCo] complex with racemic ligands. Compounds 1·sol and 1 were subjected to photomagnetic measurements by irradiation with green light (532 nm continuous wave laser) at 5 K. Indeed, both samples exhibited a moderate increase in magnetization after irradiation, followed by a gradual relaxation to the ground state as the temperature increased (Fig. 5). This behavior combined with thermally-induced polarization change suggests the possibility of light-induced polarization changes in these complexes.

Interestingly, compared to the previously reported [CrCo] complex employing a racemic ligand, the transition temperature of complex 1 is significantly lower. To understand such a discrepancy, theoretical calculations using density functional theory (DFT) were carried out at the same level of theory. Indeed, the derived energy difference of the enantiopure [CrCo] complex (0.46 kcal mol⁻¹) is significantly lower than that of the heterochiral one (3.92 kcal mol⁻¹) in the vacuum state. More careful inspection revealed that such a change mainly comes from the substantial stabilization (3.59 kcal mol⁻¹) of the HS state in the enantiopure complex, which might relate to the more distorted coordination geometry in this situation. Notably, the relative stabilization of the HS electron-transferred state in the enantiopure complex also explains the improved trapping effect in the photomagnetic measurements.55

As complex 1·sol exhibits VT behavior in the P2₁ polar space group, it is possible to realize polarization switching at a macroscopic scale. Therefore, pyroelectric measurements were performed on the single-crystal sample of compound 1·sol to investigate the electric current attributed to the variation in dipole moments during the VT transition. The well-shaped crystal was indexed, and silver paste was attached to the (010) and (0−10) surfaces that were perpendicular to the b-axis (Fig. S11†). The pyroelectric current was recorded using a Keithley 6517B electrometer without applying any external electric/magnetic field, and the temperature was controlled using a Quantum Design magnetic property measurement system in the temperature range between 30 and 250 K with a sweeping rate of 5 K min⁻¹. The current signal could be detected with opposite signs in the heating and cooling runs, certifying its pyroelectric nature. As temperature increases, the temperature-dependent pyroelectric coefficient of compound 1·sol exhibited a single broad peak centered at 162 and 174 K with a maximal value of ca. 2.9 nC cm⁻² K⁻¹ during cooling and heating processes, respectively. By integrating the pyroelectric current, the polarization change could be estimated as 0.27 μC cm⁻², and its temperature dependence shows a perfect match with the results of magnetic measurements in thermally induced polarization.

To calculate the polarization change in 1·sol theoretically, the volume average of the molecular dipole moments (0.03 and 9.16 D for triplet and septet, respectively) along the b-axis was obtained from DFT calculations. In this way, the electron-transfer contribution was estimated as 0.17 μC cm⁻², assuming that 20% of molecules (estimated from magnetic data) participate in the VT process. Besides, accompanied by the structural transition, the relative displacement between cations and anions should also contribute to polarization. This part was tentatively included by the point charge model, yielding an additional polarization change of 0.02 μC cm⁻². The net polarization change is estimated as 0.19 μC cm⁻², roughly consistent with the experimental value (0.27 μC cm⁻²) (Fig. 6). The discrepancy might result from the full negligence of the solvent orientation effects and the secondary pyroelectric effect, or inadequate consideration of the displacement contribution by an oversimplified point charge model. In any situation, it's reasonable to conclude that the observed polarization change is mainly contributed from electron transfer. As 1·sol exhibits SCSCT as confirmed by single-crystal or powder XRD, it remains interesting to investigate the solvent-induced polarization-switching behavior. Theoretically, the electron-transfer and ion-displacement contributions to polarization change could be estimated to be 0.17 and 0.00 μC cm⁻², respectively. Surprisingly, this calculated value of the electron transfer-induced polarization change is similar to that of the solvated form, owing to the opposite change caused by different degrees of VT transition and change in the projection angle. Preliminary pyroelectric measurements were also performed on the in situ desolvated sample at 310 K, which shows a clear shift in the transition temperature towards a high-temperature direction, which is consistent with the results from magnetometry (Fig. S12†). However, as the large crystal pieces required for pyroelectric measurements were more fragile than those used for single-crystal XRD measurements, and the samples consistently experienced partial cracking during the desolvation treatment, it became challenging to obtain accurate pyroelectric current data with an acceptable signal-to-noise ratio. Therefore, the polarization change of the desolvated sample remains undetermined, while the solvent effect on the polarization-switching behavior is certified by the observed temperature shift. In addition, pyroelectric measurement of 1·sol was carried out under light irradiation at 5 K. A clear opposite current in comparison with the cooling process could be observed where the electron transfers from the bridging ligand to the metal. After light was switched off, the excited state gradually decayed back to the ground state as the temperature increased where an opposite peak current was detected. This experimental observation confirmed that the polarization change of 1·sol could also be stimulated by means of light irradiation (Fig. S13†).

Conclusions

In conclusion, we presented a heterometallic dinuclear complex with an enantiopure ligand with regular molecular arrangements in a polar space group. The stepwise synthetic route proposed here successfully improves the purity of the desired crystals, and is applicable to the synthesis of other heterometallic dinuclear complexes with enantiopure ligands, even the achiral ones. Among the complexes we synthesized according to this approach, the less compact crystal packing of the hom*ochiral [CrCo] complexes offered extra space to accommodate lattice solvents compared to the situation observed in previously reported [CrCo] complexes with heterochiral ligands. Thus, a new [CrCo] complex was characterized to show a solvent-dependent VT behavior via SCSCT, as demonstrated by the single-crystal structure and magnetometry and spectroscopic techniques. Moreover, pyroelectric measurements clearly confirm the polarization-switching behavior in the pristine sample. Multi-controlled polarization switching offers a good playground for potential application in multifunctional molecular devices. Our results highlight the importance of guest molecules in polarization-switching materials, which could contribute to the further study of molecular sensors by polarization.

Author contributions

Wenwei Zheng: investigation, methodology, conceptualization and writing – original draft; Xiaopeng Zhang: investigation and validation; Qirui Shui, Tatsuki f*ckuyama, Wen-Huang Xu, Yu-Bo Huang, Tianchi Ji, Ziqi Zhou, and Mikoto Uematsu: investigation; Sheng-Qun Su: methodology, writing – review and editing, and funding acquisition; Shinji Kanegawa: methodology, writing – review and editing, and funding acquisition; Shu-Qi Wu: formal analysis, conceptualization, writing – review and editing, and funding acquisition; Osamu Sato: supervision, project administration, writing – review and editing, and funding acquisition.

Conflicts of interest

There are no conflicts to declare.

Acknowledgements

This work was supported by JSPS KAKENHI (21K05085, 22K14694, 20H00385, 21K05086, 23H04862, 24H00466, and 24K17698). S.-Q. W. and S.-Q. S. are grateful for the support from the Iketani Science and Technology Foundation (0341056A and 0351039A).

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