Abstract
Quantum entanglement in magnetic materials is expected to yield a quantum spin liquid (QSL), in which strong quantum fluctuations prevent magnetic ordering even at zero temperature. This topic has been one of the primary focuses of condensedmatter science since Anderson first proposed the resonating valence bond state in a certain spin1/2 frustrated magnet in 1973. Since then, several candidate materials featuring frustration, such as triangular and kagome lattices, have been reported to exhibit liquidlike behavior. However, the mechanisms that stabilize the liquidlike states have remained elusive. Here, we present a QSL state in a spin1/2 honeycomb lattice with randomness in the exchange interaction. That is, we successfully introduce randomness into the organic radialbased complex and realize a randomsinglet (RS) state (or valence bond glass). All magnetic and thermodynamic experimental results indicate the liquidlike behaviors, which are consistent with those expected in the RS state. Our results suggest that the randomness or inhomogeneity in the actual systems stabilize the RS state and yield liquidlike behavior.
Introduction
A quantum spin liquid (QSL) is one of the fascinating ground states encountered in the field of condensed matter physics. In a QSL, enhanced quantum fluctuations in strongly correlated spins prevent magnetic ordering, inducing the formation of a disordered state that exhibits liquidlike spin behavior. Anderson proposed the resonating valence bond as a possible QSL state in the S = 1/2 frustrated triangular lattice^{1}. Following considerable experimental research, several candidate materials have since been reported. For example, the organic salts κ–(BEDTTTF)_{2}Cu_{2}(CN)_{3} ^{2,3,4} and EtMe3Sb[Pd(dmit)_{2}]_{2} ^{5,6}, which form S = 1/2 Heisenberg antiferromagnetic (AF) triangular lattices are known to be promising candidates. These materials have no magnetic order down to very low temperatures and exhibit gapless (or nearly gapless) behaviors. However, theoretical research has established that the ground state of the triangular lattice is an AF ordered state^{7,8}. Thus, the true origin of the liquidlike behavior observed in these organic salts remains an open question.
Subsequent theoretical studies on the triangular lattice with the liquidlike behavior have revealed several mechanisms that may stabilize a QSL state. The numerical calculations employed in those investigations incorporate additional effects that are neglected in the simplest model with nearestneighbor bilinear coupling^{9,10,11}. Meanwhile, it has been noted that the inhomogeneity in the actual systems, which causes spatially random exchange coupling (bondrandomness), may be essential for the observed liquidlike behavior^{12,13}. As regards organic salts, strong coupling between the spin and electric polarization at each spin site and its importance to the liquidlike behavior have been noted^{14,15}. In the lowtemperature region, a random freezing of the electiric polarization is indicated by the glassy response in the dielectri properties^{16,17}. Accordingly, the spindensity distribution at each lattice site should be also randomly freezing and causes the bondrandomness.
Recent numerical analysis of the bondrandomness effect on an S = 1/2 Heisenberg AF triangular lattice has revealed that sufficiently strong randomness stabilizes a gapless QSL state^{12,13}. Such a randomnessinduced QSL, in which spinsinglet dimers of varying strengths are formed in a spatially random manner, corresponds to a socalled randomsinglet (RS) or valencebond glass (VBG)^{18,19}. Because the exchange interactions are randomly distributed, the binding energy of the singlet dimers has a wide distribution, yielding gapless behavior. The RS (or VBG) state is expected to exhibit liquidlike behaviors characterized by a Tlinear specific heat, a gapless susceptibility with an intrinsic Curie tail, a nearlinear magnetization curve^{12,20}. Indeed, many of the experimentally observed liquidlike behaviors of the triangular organic salts are explained by the RS picture. In the case of an S = 1/2 Heisenberg AF honeycomb lattice, which is our focus in this letter, the groundstate phase diagram for the bondrandomness versus frustration is investigated^{21}. It is suggested that liquidlike behavior can be realized even in the case of very weak frustration. Although some honeycomblatticebased compounds have recently been reported to exhibit liquidlike behavior, their exact lattice systems have not been clarified^{22,23}. In this work, we present a new S = 1/2 Heisenberg AF honeycomb lattice composed of three dominant interactions, as shown in Fig. 1a. Those interactions are designed to have bondrandomness with a weak additional AF interaction J _{4} inducing frustration in the lattice. Our experimental results regarding the magnetic and thermodynamic properties indicate the realization of the RS state, as schematically shown in Fig. 1b.
Recently, we developed verdazyl radical systems with flexible molecular orbitals (MOs) that enable tuning of the intermolecular magnetic interactions through molecular design^{24,25,26}. In this study, we utilized a new verdazylbased complex Zn(hfac)_{2}(A_{ x }B_{1−x }), where hfac represents 1,1,1,5,5,5hexafluoroacetylacetonate, and A and B equivalent to regioisomers of verdazyl radical. It is essential for introduction of randomness that the rotational degrees of freedom of verdazyl radical disappear owing to the coordination to Zn(hfac)_{2}, as shown in Fig. 2a. Accordingly, two different regioisomers, labeled Atype (x) and Btype (1x), arise and randomly align in the crystal, yielding randomness of the intermolecular exchange interactions.
The randomness effect reaches maximum at x = 0.5, where the numbers of A and Btype molecules are identical. Some numerical inequalities exist depending on the conditions of the solution used in the complexforming reaction (see Method section), and the actual crystals have slightly large x values. Here, we successfully synthesized two different single crystals with x = 0.64 and 0.79. The crystallographic parameters were determined at room temperature and 25 K for both crystals (Supplementary Table S1). Only slight differences were observed between the results for x = 0.64 and 0.79. Note that, because this investigation focused on the lowtemperature magnetic properties, the crystallographic data at 25 K are discussed hereafter. The crystallographic parameters at 25 K for x = 0.64 were as follows: monoclinic, space group P2_{1}/n, a = 9.010(3) Å, b = 31.640(11) Å, c = 10.902(4) Å, V = 3107.8(19) Å, Z = 4. We performed the MO calculations and found three types of dominant interactions, i.e., J _{1}, J _{2}, and J _{3}, and an additional weak interaction J _{4}, as shown in Fig. 1a. The molecular pairs associated with those exchange interactions are all related by inversion symmetry, as shown in Fig. 2b–e.
Considering the A and Btype molecule combination with the inversion center between them, each interaction has three pair formation patterns, i.e., AA, AB (=BA), and BB. We focused on the x = 0.64 crystal as it has a stronger randomness effect. The AA, AB, and BB pairs have possibilities of x ^{2} = 0.41, 2x(1−x) = 0.46, (1−x)^{2} = 0.13, respectively. The exchange interactions J _{ i }/k _{B} = {AA, AB, BB} (i = 1–4; k _{ B } is the Boltzmann constant) were evaluated as J _{1}/k _{B} = {−9.5 K, −14.5 K, −15.8 K}, J _{2}/k _{B} = {7.2 K, 7.1 K, 6.9 K}, and J _{3}/k _{B} = {3.9 K, 7.8 K, 10.0 K}; these terms are defined in the Heisenberg spin Hamiltonian given by \( {\mathcal H} ={J}_{n}{\sum }_{ < i,j > }{S}_{i}\cdot {S}_{j}\), where \({\sum }_{ < i,j > }\) denotes the sum over the corresponding spin pairs. Note that J _{4}/k _{B} is almost independent of the pair formation and evaluated to be 0.08 K.
Figure 3a shows the temperature dependence of the magnetic susceptibilities (χ = M/H) for various magnetic fields. Although we performed fieldcooled and zerofieldcooled measurements to examine spinfreezing for x = 0.64, no distinguishable differences were found (Fig. 3a). Below 0.25 T, a shoulder is apparent at approximately 1 K, along with gapless behavior with a Curie tail in the lower temperature region, for both x = 0.64 and 0.79. This shoulder indicates development of AF correlations forming spinsinglet dimers, and the Curielike diverging components indicate a small fraction of free spins owing to some unpaired gorphan h spins, as illustrated in Fig. 1b. The appearance of the small freespin fraction generating Curielike lowtemperature χ is indeed expected in the RS picture^{12,20,21}.
The magnetization curves at the lowest temperature of 0.08 K also indicate gapless behaviors, as shown in Fig. 3b. The entire magnetization curve for x = 0.64 exhibits the nearlinear behavior expected for the RS state^{12}, whereas that for x = 0.79 exhibits slight bending at approximately 3.5 T. Such bending was also observed in the magnetization curve calculated for the RS state near the saturation field^{12,20}. In general, there is a sharp change in the magnetization curve at the saturation field for nonrandomness phase. By introducing bondrandomness, the magnetization curve near the saturation field becomes gradual, originating from the widely distributed binding energy of the singlet dimers. That is, bending appears when the randomness is small. When the randomness is increased, the bending eventually becomes almost linear. As the randomness increases when x approaches 0.5, the nearlinear behavior in the magnetization curve for x = 0.64 is consistent with the theoretical prediction for RS state.
The temperature dependence of the specific heat, C _{p}, for x = 0.64 is shown in Fig. 4. In the lowtemperature regions below 0.5 K, a clear gapless Tlinear behavior was observed, C _{p} \(\simeq \,\gamma T\). This Tlinear behavior is robust against an applied magnetic field and appears even under a highmagnetic field near the saturation field. Such Tlinear behavior of the specific heat is consistent with the specific heat expected in the RS picture^{21}, which originates from the widely distributed binding energy. We also found a broad hump structure in the temperature dependence of C _{p}/T (Fig. 4, inset). Note that similar broad hump structures have also been observed for the C _{p}/T/ of organic triangular salts, in which the broad hump is considered to be a crossover to QSL state^{3,6}. We roughly evaluated γ from the C _{p}/T values at the lowest temperatures and obtained 1.20 and 0.72 J/mol K^{2} at 0 and 3 T, respectively. From numerical analysis of the RS state, we thus deduced that the Tlinear term of C _{p} is strongly dependent on the fundamental ground state without randomness and, also, on the degree of introduced randomness^{12,20,21}. The obtained γvalues are somewhat large, but do not differ significantly from the calculations.
In the honeycomb lattice, a relatively small lattice distortion can induce a disordered gapped phase (even in the nonfrustrated case) owing to strong quantum fluctuation^{27,28}. From the theoretical analysis, it is deduced that the introduction of bondrandomness into the gapped phases is more effective for RS state formation than introduction into the gapless ordered phase^{12,20,21}. Therefore, in the present model, the lattice distortion as well as the weak frustrated interaction should enhance the bondrandomness effect, inducing formation of the RS state.
In summary, we have succeeded in synthesizing single crystals of the verdazylbased complex Zn(hfac)_{2}(A_{ x }B_{1−x }). Two different regioisomers, Atype (x) and Btype (1x), arise and randomly align in the crystal, yielding randomness of the intermolecular exchange interactions. Ab inotio MO calculations indicate the formation of the S = 1/2 Heisenberg AF honeycomb lattice composed of three dominant interactions, and there is a weak additional AF interaction inducing frustration in the lattice. All magnetic and thermodynamic experimental results indicate the liquidlike behaviors, which are consistent with those expected in the RS state, These results demonstrate that the randomness or inhomogeneity in the actual systems stabilize the RS state and yield liquidlike behavior. Furthermore, our method to introduce a bondrandomness into spin lattices enable further investigations on the randomnessinduced QSL in other lattice systems.
Methods
We synthesized Zn(hfac)_{2}(A_{ x }B_{1−x }) using a conventional procedure similar to that used to prepare the typical verdazyl radical 1,3,5triphenylverdazyl^{29}. A solution of pCloPyV [1(4chlorophenyl)3(2pyridyl)5phenylverdazyl] (119 mg, 0.34 mmol) in 10 ml of CH_{2}Cl_{2} was slowly added to a solution of [Zn(hfac)_{2}]·2H_{2}O (175 mg, 0.34 mmol) in 20 ml of heptane at 80 °C, and stirred for 1 h. After the mixed solution cooled to room temperature, a darkgreen crystalline solid of Zn(hfac)_{2}(A_{ x }B_{1−x }) was separated by filtration and washed with pentane. The darkgreen residue was recrystallized using CH_{2}Cl_{2} in an acetonitrile atmosphere. The crystal structure was determined on the basis of intensity data collected using a Rigaku AFC8R Mercury CCD RAMicro7 diffractometer with a Japan Thermal Engineering XRHR10K. The magnetizations were measured down to approximately 80 mK using a commercial SQUID magnetometer (MPMSXL, Quantum Design) and a capacitive Faraday magnetometer. The experimental results were corrected for diamagnetic contributions (−4.2 × 10^{−4} emu mol^{−1} for x = 0.64 and −4.0 × 10^{−4} emu mol^{−1} for x = 0.79), which were determined to become almost χT = const. above approximately 200 K, and close to the value calculated using Pascal’s method. The specific heat was measured using a handmade apparatus and a standard adiabatic heatpulse method down to ∼0.1 K. Considering the isotropic nature of organic radical systems, all experiments were performed using small randomly oriented single crystals. The ab initio MO calculations were performed using the UB3LYP method as brokensymmetry hybriddensity functional theory calculations. All the calculations were performed using the Gaussian 09 program package, with the basis functions being 6–31G. To estimate the intermolecular magnetic interaction of the molecular pairs, we applied our previously presented evaluation scheme^{30}.
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Acknowledgements
We thank T. Kawakami for valuable discussions. This research was partly supported by KAKENHI (No. 17H04850, No. 15H03682, and No. 15H03695). Part of this work was performed as a jointresearch program involving the Institute for Solid State Physics (ISSP), the University of Tokyo, and the Institute for Molecular Science.
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H.Y. and M.O performed sample preparation and characterization. H.Y., Y.K., T.O., Y.I., and Y.H. discussed the results. H.Y., M.O., Y.K., S.K., T.S., and Y.I. performed the experiments.
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Yamaguchi, H., Okada, M., Kono, Y. et al. Randomnessinduced quantum spin liquid on honeycomb lattice. Sci Rep 7, 16144 (2017). https://doi.org/10.1038/s41598017164310
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DOI: https://doi.org/10.1038/s41598017164310
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