Metal-free liquid-crystalline (LC) materials consisting of a LC nitroxide radical compound exhibit light-induced reversible switching of the magnetic properties as a new photomagnetic effect. This behavior is based on the abrupt change of magnetic properties at the phase transition directly from a chiral smectic C phase to an isotropic liquid (Iso) phase. The origin of the abrupt change is probably the difference in the inhomogeneity of the intermolecular magnetic interactions between LC and Iso phases. To our knowledge, there are no existing reports on a material showing the reversible and quick phase transitions with the large difference of the inhomogeneity. Here we show a relatively simple way to design a compound to enlarge the difference between LC and Iso phases and to make the response quick and reversible. In addition, the presented analysis method that mines Gaussian components from electron paramagnetic resonance spectra enables us to precisely evaluate magnetic properties in condensed phases.
Liquid-crystalline (LC) materials show high responsivity to various stimuli due to their collective molecular motion1. The high responsivity can lead to developments of LC devices; in fact, LC displays need the control of light propagation by means of the molecular reorientation in applied electric fields2. Conversely, the properties of LC materials can strongly respond to light stimuli; e.g., azobenzene-based or doped LC materials show photo-fluidization3,4, which induces developments of self-healing abilities of composite gels5, remote-controllable light shutters6, light-controllable soft actuators7,8, and image storages9,10. It had been natural that magnetic properties of metal-free compounds are undetectably weak in high-temperature LC phases unlike the above-mentioned properties until some metal-free LC compounds with a stable nitroxide radical moiety in the mesogen core or as one of the terminal groups (LC-NRs) were reported to exhibit the detectable change in magnetic properties at their melting points (Fig. 1a)11,12,13,14,15,16,17,18,19.
Despite the radical moiety, LC-NRs are thermally stable up to about 150 °C in the air and in water, and a lot of analogs showing a variety of LC phases have been reported11,14,15,17,20,21,22,23,24,25,26. Moreover, spin glass-like inhomogeneous magnetic interactions occur in fluid (Fl) phases: LC and isotropic (Iso) phases13. The difference in the inhomogeneity of the interactions is likely to result in that in the magnetic properties. Since crystalline (Cr) phases have uniform intermolecular interactions, whereas Fl phases have the most inhomogeneous ones13,14, the abrupt large changes of magnetic properties occur only at Cr-to-Fl phase transitions thus far13,14,15,17,18. However, such transitions from or to Cr phases are usually irreversible and/or too slow. In contrast, since LC-to-Iso phase transitions, which are transitions between Fl phases, are reversible and fast, these can immediately occur in response to external stimuli like not only temperature but also light. Thus, LC materials consisting of the magnetic LC compounds could exhibit light-induced reversible switching of magnetic properties as a new photomagnetic effect (Fig. 1b). However, since the magnetic properties of the previously reported LC-NRs hardly change at the LC-to-Iso phase transitions12,13,14,15,16,17,18,19, we have to design a new compound showing the large change of magnetic properties at the LC-to-Iso phase transitions to realize the light-induced reversible switching.
Organic chemists can concisely design molecules in the order of atoms specially for the target stimulus to which LC materials responds; the simplest way to design such a compound is to enlarge the difference in the inhomogeneity of the intermolecular magnetic interactions between LC and Iso phases in terms not only of orientational order14 but also of one- or two-dimensional (1-D or 2-D) positional order. We focused on rod-like mesogens with more than three side chains, so-called forked structure; the nanophase separation of flexible aliphatic chains from rigid aromatic units results in a high layer order in their LC phases27. Accordingly, an LC-NR with the forked structure could show high orientational and layer, that is 1-D positional, orders in LC phases that should induce the large abrupt change of magnetic properties at the LC-to-Iso phase transition.
Here, we report the synthesis of the first example of LC-NRs to the best of our knowledge, with the forked structure as shown in Fig. 1a. The changes of magnetic properties at the temperature-induced phase transitions in the forked LC-NRs (2S,5S)-8NO82 and (±)-8NO82 are evaluated by means of superconducting quantum interference device (SQUID) magnetometry and variable-temperature electron paramagnetic resonance (VT-EPR) spectroscopy. We demonstrate the photomagnetic effect of metal-free LC materials consisting of (2S,5S)-8NO82 and an azobenzene analog. In addition, in the course of the analysis of the VT-EPR spectra, a more detailed analysis method for magnetic properties unique to LC phases has been developed to discuss the temperature dependence of paramagnetic susceptibility with high accuracy and the influence of the inhomogeneous intermolecular contacts in detail.
Compounds (2S,5S)-8NO82 and (±)-8NO82 were prepared by the synthetic procedure shown in Supplementary Fig. 1 and characterized by high performance liquid chromatography (HPLC) analysis, infrared (IR) spectroscopy, nuclear magnetic resonance (NMR) spectroscopy, and high resolution mass spectrometry (HRMS) (Supplementary Figs. 2–5). The phase transition temperatures of (2S,5S)-8NO82 and (±)-8NO82 were determined by differential scanning calorimetry (DSC) at a scanning rate of 2 °C/min upon first heating and cooling processes as shown in Supplementary Fig. 6, variable temperature X-ray diffraction (VT-XRD) analyses in the first heating process as shown in Supplementary Figs. 7 and 8, and polarized optical microscopy (POM) as shown in Supplementary Fig. 9; (2S,5S)-8NO82 shows an enantiotropic chiral smectic C (SmC*) phase between 44.3 °C and 53.8 °C, and (±)-8NO82 shows a monotropic smectic C (SmC) phase (see Supplementary Discussion). The chiral nematic (N*) and nematic (N) phases for (2S,5S)-8NO8 and (±)-8NO8 are replaced with SmC* and SmC phases for (2S,5S)-8NO82 and (±)-8NO82, respectively11, owing to the additional octyloxy side chain. The nanophase separation between incompatible parts of the forked mesogens, abundant flexible aliphatic chains and rigid aromatic units, is likely to induce layer order and biaxiality27.
In addition, it is worth noting that 8NO82 have larger transition enthalpy ∆H (~4.5 times) and transition entropy ∆S (~5 times) at the clearing points than 8NO8 as summarized in Table 1. The increase of ∆H indicates that the forked mesogens 8NO82 have larger intermolecular interactions which induce both higher orientational and layer ordering in the SmC* and SmC phases. Furthermore, the increase of ∆S indicates that 8NO82 has the fewer number of possible conformations and configurations in the SmC* and SmC phases than 8NO8 in N* and N phases if the conformations and configurations are equally random in both the Iso phases of 8NO8 and 8NO82. Therefore, it is easy to anticipate that the inhomogeneity of the intermolecular contacts sharply increases at the LC-to-Iso phase transition of 8NO82; the large abrupt change of paramagnetic susceptibility could occur at the phase transition.
Detailed insight into SmC* structure
VT-XRD measurements allow the calculation of the translational order parameter Σ, so-called smectic order parameter, providing information of the quality of the translational periodicity of the smectic layers, and the correlation length ξ for the smectic ordering (Supplementary Discussion and Supplementary Figs. 10 and 11). The temperature dependence of Σ in the SmC* phase of (2S,5S)-8NO82 can be estimated from the integrated temperature-dependent scattering intensity AXRD(T) of the peak for (001) according to previously developed method (see Supplementary Methods)28. The experimental AXRD(T) data are well reproduced by Eq. (1) as shown in Supplementary Fig. 10 with the values of TC = 3.2733(3) × 102 K, AXRD0 = 1.88(1) × 104, and β = 3.48(7) × 10–2, which are comparable with the previously reported experimental values for SmC* materials28.
The obtained Σ value for (2S,5S)-8NO82 is larger than that for conventional thermotropic LC compounds, which usually ranges around 0.7, as shown in Fig. 228,29. It implies that the molecules are rarely dislocated out of the smectic layers. The specificity in Σ value of (2S,5S)-8NO82 perhaps reflects both steric aggregability of side chains arising from intercalation to reduce free volume and electrostatic aggregation of rigid cores originating from large lateral dipole on the nitroxide. It reminds us that the similar situation of compounds showing high Σ value around 0.9 possesses specific side groups such as siloxane30,31,32, fluorinated carbon groups32, polar groups32, and ionic moiety33,34, which strongly repel rigid core and/or attract adjacent side chains.
To compare the magnetic properties in the Cr, LC, and Iso phases, first, we have to confirm the magnetic interactions in the Cr phases because the magnetic properties in Cr phase serve as references for those in Fl phases. Molar magnetic susceptibility χM for (2S,5S)-8NO82 and (±)-8NO82 is available by means of SQUID magnetometry in a magnetic field of 0.5 T in the temperature range of 2–300 K in the first heating process. The obtained results indicate that the NO groups are chemically stable and that the crystals of (2S,5S)-8NO82 and (±)-8NO82 show weak intermolecular antiferromagnetic interactions at low temperature (θ < 0 and J < 0, Supplementary Fig. 12, Supplementary Table 1 and Supplementary Discussion).
In turn, we measured the temperature dependence of paramagnetic susceptibility χpara of (2S,5S)-8NO82 between 313 and 340 K (40 and 67 °C) by means of SQUID magnetometry in a magnetic field of 0.05 T (Fig. 3). The χpara–T and χparaT–T plots seem to obey the Curie–Weiss law in the temperature range between 313 and 327 K, where Curie constant C = 0.398 emu K mol−1 and Weiss constant θ = −0.032 K, respectively. The χpara value seems mostly unchanged at the Cr-to-SmC* phase transition. In contrast, the experimental χpara of (2S,5S)-8NO82 in the Iso phase is larger than that estimated from the Curie and Weiss constants for the lower-temperature phases; χpara and χparaT increase at the SmC*-to-Iso phase transition (1.7% at 330 K in 0.05 T) as shown in Fig. 3, which is referred to as the positive magneto-LC effect15. As expected, the change ratios of the χpara values at the Cr-to-LC and LC-to-Iso phase transitions for (2S,5S)-8NO82 are unusual; previously reported LC-NRs show larger change ratios at Cr-to-LC phase transitions than those at LC-to-Iso phase transitions.
A clue to the origin of these new phenomena should come from a close examination of the difference in intermolecular interactions between the phases by means of EPR spectroscopy (Supplementary Fig. 13), which also gives the temperature dependence of χpara13,14. To improve the accuracy to estimate the temperature dependence of χpara, we have developed the following method; the experimental EPR spectra are fitted with the area-normalized pseudo-Voigtian derivative instead of Lorentzian derivative used in the previously reported method (see Supplementary Figs. 14 and 15)13. The new method excels in the deconvolution of experimental EPR spectra and can include Gaussian contributions in χpara values with high accuracy (see Supplementary Discussion)14. The temperature dependence of relative paramagnetic susceptibility χrel for (2S,5S)-8NO82 showed a small χrel increase by 0.55% at the Cr-to-SmC* phase transition (from 45 to 47 °C) as shown in Fig. 3c. Moreover, it is noteworthy that χrel increased by 3.7% at the SmC*-to-Iso phase transition (from 55 to 56 °C), which is larger than that at the Cr-to-SmC* phase transition. These phenomena are consistent with those from SQUID magnetometry (Fig. 3a). Among all NR compounds, (2S,5S)-8NO82 shows the largest increase of χpara at the LC-to-Iso phase transition. For the LC-NRs, the anisotropy of paramagnetic susceptibility ∆χpara, which is theoretically proportional to the anisotropy of g2, does not seem to cause the changes of χrel as shown in Fig. 3d (see Supplementary Discussion). This unfamiliar trend is likely to be attributed to the LC nature of (2S,5S)-8NO82, which is similar to the Cr phase rather than the Iso phase. In addition, (±)-8NO82 also shows the similar phenomena at the phase transition to the Iso phase in the heating process (Supplementary Fig. 16).
Next, the correlation between the temperature dependence of χrel and that of the parameters estimated from EPR spectra should give an interpretation of the phenomena (Fig. 3). The deconvolution of the Voigtian EPR spectra gives two types of temperature-dependent peak-to-peak linewidths, Lorentzian linewidth ∆BppL and Gaussian linewidth ∆BppG as shown in Fig. 3. Generally, ∆BppL reflects the following two magnetic interactions: (a) spin–spin dipolar interactions (the stronger the interaction is, the more the ∆BppL increases) and (b) spin–spin exchange interactions (the stronger the interaction is, the more the ∆BppL decreases)13,15. Meanwhile, ∆BppG reflects the inhomogeneous broadening of the EPR spectra, which is useful to discuss the contribution of the inhomogeneity of the intermolecular magnetic interactions to the magneto-LC effects14.
The temperature dependence of ∆BppL around the SmC*-to-Iso phase transition is different from that around the Cr-to-SmC* phase transition; the abrupt large increase in ∆BppL occurred in concert with the abrupt increase in χrel at the SmC*-to-Iso phase transition in the heating process (Fig. 3), indicating the generation of ferromagnetic spin–spin dipolar interactions in the Iso phase and/or the extinction of antiferromagnetic spin–spin exchange interactions. The delicate balance of the two factors is likely to give rise to the complicated behavior of temperature dependence of ∆BppL. However, we could say that ∆BppG is the dominant factor for the χrel change (Fig. 3). The large increase of ∆BppG at the SmC*-to-Iso phase transition indicates that the additional appearance of inhomogeneity of intermolecular magnetic interactions in the Iso phase. These results suggest that the intermolecular magnetic interactions can become more inhomogeneous even at the SmC*-to-Iso phase transition, and the averaged ferromagnetic interactions further increase in the Iso phase.
To gain an insight into the origin of the changes of χrel, ∆BppL, and ∆BppG at SmC*-to-Iso phase transition, we have to focus on the structural details of intermolecular contacts in these Fl phases. The estimated correlation length ξ for the smectic ordering (Supplementary Fig. 12) indicates that molecules contact with each other in the same manner in the range up to about 80 nm in length. Based on the tendency that the intermolecular magnetic interactions between nearest molecules dominate magnetic properties of organic radicals with localized spins35, it can be considered that the 80 nm is much longer in terms of intermolecular magnetic interactions. Thus, the intermolecular magnetic interactions are considered to be sufficiently homogeneous in the SmC* phase of (2S,5S)-8NO82. In addition, the high smectic order parameter Σ of (2S,5S)-8NO82 even in the vicinity of Iso-to-SmC* phase transition (Fig. 2) implies that the molecules in the SmC* phase are little dislocated out of the layers and are arranged in Cr-like manner. And this high Σ is consistent with large transition entropy ∆S at SmC*-to-Iso phase transition (Table 1). These results mean that the intermolecular magnetic interactions in the SmC* phase of (2S,5S)-8NO82 are similar to those in the Cr phase over the whole system. Thus, the loss of the Cr-like layer order in the SmC* phase should induce the large increase of inhomogeneity of the intermolecular contacts and of averaged intermolecular ferromagnetic interactions, leading to the large abrupt change of χrel, at the SmC*-to-Iso phase transition. Therefore, as a guideline to prepare LC-NRs showing large increases of χpara at LC-to-Iso phase transitions, additional aliphatic side chain is likely to be effective because it induces not only orientational order but also high layer order in the LC phases.
Reversible switching of magnetic properties
With the effective use of this large change of magnetic properties at SmC*-to-Iso phase transition, temperature change could induce the reversible switching of magnetic properties. The parameters estimated from EPR spectra for (2S,5S)-8NO82 at TCP − 2 = 52 °C and TCP + 2 = 56 °C, where TCP is a clearing point, are different from each other; e.g., χrel increases by 4.5% as temperature increases from 52 to 56 °C, and it returns to the initial value as temperature returns (Fig. 4a). In contrast to conventional solid-state magnetic materials showing a decrease of magnetic susceptibility with increasing temperature, it is noteworthy that (2S,5S)-8NO82 exhibits an increase of magnetic susceptibility with increasing temperature. Besides, the absolute value of the variation of χrel for (2S,5S)-8NO82 (4.5%) is much larger than that expected from Curie law for usual paramagnetic materials (1.2%) (see Supplementary Discussion). Furthermore, all the parameters of (2S,5S)-8NO82 also show reversible switching (Fig. 4b–d). These results indicate that the changes of inhomogeneity of intermolecular magnetic interactions through the temperature-change-induced phase transitions contribute to the magnetic switching as mentioned above and that (2S,5S)-8NO82 is stable against repeated heating and cooling processes.
We focused on light irradiation as one of the other external stimuli to induce the SmC*-to-Iso and Iso-to-SmC* phase transitions because light stimuli can be controlled much more quickly than temperature. According to previous reports3,9, for the photo-induced switching of the magnetic properties, we doped 4-butyl-4′-methoxyazobenzene (BMAB) into (2S,5S)-8NO82 by 5.1 mol% (Fig. 5 and Supplementary Fig. 17). It induces photo-fluidization originating from photoisomerization of the azobenzene moiety; the UV and visible lights cause its trans-to-cis and cis-to-trans photoisomerization, respectively (see Supplementary Methods)3,9. The phase transition of the photo-responsive magnetic LC mixture was characterized by POM (Supplementary Fig. 18) and DSC (Supplementary Fig. 19) analyses (see Supplementary Discussion). The mixture shows an enantiotropic SmC* phase from room temperature to 51.2 °C in the DSC chart; the doped BMAB does not extinguish the intrinsic LC nature of (2S,5S)-8NO82. Actually, we confirmed that the UV light (365 nm) and visible light (530 nm) repeatedly induce SmC*-to-Iso and Iso-to-SmC* phase transitions at 52.4 °C in the POM, respectively. To find the most appropriate temperature for the photo-induced magnetic switching, we measured the temperature dependence of paramagnetic susceptibility of the photo-responsive magnetic LC mixture in dark or under UV light irradiation by means of EPR spectroscopy. The χrel abruptly increased at 52 °C in dark, whereas it gradually increased around 45 °C under UV light irradiation (Fig. 5). The variation of the transition temperature should be attributed to the variation of the concentration of cis isomer of BMAB. The most appropriate temperature is likely to be 51 °C.
We examined if the photo-induced magnetic switching occurs in the LC mixture at 51 °C as shown in Fig. 5 (Supplementary Fig. 20). All magnetic properties reversibly change under the UV and visible light irradiation; the behavior resembles the temperature-change-induced switching (Fig. 4). These results also indicate that both (2S,5S)-8NO82 and BMAB are stable under the UV irradiation. We can conclude that the photo-induced SmC*-to-Iso and Iso-to-SmC* phase transitions causes the magnetic switching as shown in Fig. 1b; in fact, the changes of magnetic properties were too small to be recognized at 60 °C, where Iso phase is the most stable even under visible light irradiation. This is the first example of photomagnetic effects in condensed fluid phases of organic radicals above room temperature.
We have successfully prepared a magnetic soft material showing light-responsive magnetic properties, which consists mainly of a chiral nitroxide radical (2S,5S)-8NO82 showing a highly ordered SmC* phase. Its forked mesogen is likely to induce strong magneto-LC effects at the SmC*-to-Iso phase transition. The switching of magnetic properties is reversible and stable against repeated irradiation of light as well as temperature change. Besides, in principle, the switching by applying electric fields would be also possible if the SmC* phase shows ordered polarization states like ferroelectric or antiferroelectric state when it is introduced into a thin cell16. In general, the induction of highly ordered LC phases is crucial to this system. The large responsivity due to the collective molecular motion in LC phases, which is not available in solid phases, results in these unique magnetic properties switchable by various external stimuli. The design of magnetic soft materials, which utilizes the large abrupt change of magnetic properties at LC-to-Iso phase transition, has potential to open new routes to materials with potentially useful applications. In addition, the discussed analysis method, which mines Gaussian components from EPR spectra, enables us to evaluate magnetic properties in fluid phases.
Characterization of LC-NRs
Phase transition of LC-NRs
Translational order parameters in the SmC* phase
Tilt angles in the SmC* phase
See Supplementary Methods.
Correlation lengths in the SmC* phase
Evaluation of magnetic properties from SQUID magnetometry
Derivation of magnetic properties from EPR spectroscopy
Preparation of photo-responsive magnetic LC mixture
Phase transition of photo-responsive magnetic LC mixture
Photo-responsive magnetic properties
Data and code availability
All data generated during the current study are available in this article and the Supplementary Information file or from the corresponding author on reasonable request.
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The authors extend appreciation to Professor Rui Tamura, Kyoto University, for experimental support, including measurement of X-ray diffraction and to Ms. Kaho Yamamoto, Osaka University, for assistance at making fitting programs. This work was supported in part by the Japan Science and Technology Agency (JST) ‘Precursory Research for Embryonic Science and Technology (PRESTO)’ for a project of ‘Molecular technology and creation of new function’ and by JSPS KAKENHI Grant Number JP17H04896. T.A. is very grateful to the JSPS Research Fellowships for Young Scientists JP16J05585. The computations were performed using Research Center for Computational Science, Okazaki, Japan.
The authors declare no competing interests.
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Akita, T., Sugiyama, Y., Yamazaki, T. et al. Photomagnetic effects in metal-free liquid crystals. Commun Chem 2, 64 (2019). https://doi.org/10.1038/s42004-019-0165-9
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