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# Randomness-induced quantum spin liquid on honeycomb lattice

## 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 condensed-matter science since Anderson first proposed the resonating valence bond state in a certain spin-1/2 frustrated magnet in 1973. Since then, several candidate materials featuring frustration, such as triangular and kagome lattices, have been reported to exhibit liquid-like behavior. However, the mechanisms that stabilize the liquid-like states have remained elusive. Here, we present a QSL state in a spin-1/2 honeycomb lattice with randomness in the exchange interaction. That is, we successfully introduce randomness into the organic radial-based complex and realize a random-singlet (RS) state (or valence bond glass). All magnetic and thermodynamic experimental results indicate the liquid-like 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 liquid-like 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 liquid-like spin behavior. Anderson proposed the resonating valence bond as a possible QSL state in the S = 1/2 frustrated triangular lattice1. Following considerable experimental research, several candidate materials have since been reported. For example, the organic salts κ–(BEDT-TTF)2Cu2(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 state7,8. Thus, the true origin of the liquid-like behavior observed in these organic salts remains an open question.

Subsequent theoretical studies on the triangular lattice with the liquid-like 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 nearest-neighbor bilinear coupling9,10,11. Meanwhile, it has been noted that the inhomogeneity in the actual systems, which causes spatially random exchange coupling (bond-randomness), may be essential for the observed liquid-like behavior12,13. As regards organic salts, strong coupling between the spin and electric polarization at each spin site and its importance to the liquid-like behavior have been noted14,15. In the low-temperature region, a random freezing of the electiric polarization is indicated by the glassy response in the dielectri properties16,17. Accordingly, the spin-density distribution at each lattice site should be also randomly freezing and causes the bond-randomness.

Recent numerical analysis of the bond-randomness effect on an S = 1/2 Heisenberg AF triangular lattice has revealed that sufficiently strong randomness stabilizes a gapless QSL state12,13. Such a randomness-induced QSL, in which spin-singlet dimers of varying strengths are formed in a spatially random manner, corresponds to a so-called random-singlet (RS) or valence-bond 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 liquid-like behaviors characterized by a T-linear specific heat, a gapless susceptibility with an intrinsic Curie tail, a near-linear magnetization curve12,20. Indeed, many of the experimentally observed liquid-like 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 ground-state phase diagram for the bond-randomness versus frustration is investigated21. It is suggested that liquid-like behavior can be realized even in the case of very weak frustration. Although some honeycomb-lattice-based compounds have recently been reported to exhibit liquid-like behavior, their exact lattice systems have not been clarified22,23. 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 bond-randomness 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 design24,25,26. In this study, we utilized a new verdazyl-based complex Zn(hfac)2(A x B1−x ), where hfac represents 1,1,1,5,5,5-hexafluoroacetylacetonate, 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 A-type (x) and B-type (1-x), 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 B-type molecules are identical. Some numerical inequalities exist depending on the conditions of the solution used in the complex-forming 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 low-temperature 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 P21/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 B-type molecule combination with the inversion center between them, each interaction has three pair formation patterns, i.e., A-A, A-B (=B-A), and B-B. We focused on the x = 0.64 crystal as it has a stronger randomness effect. The A-A, A-B, and B-B 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 = {A-A, A-B, B-B} (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 field-cooled and zero-field-cooled measurements to examine spin-freezing 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 spin-singlet dimers, and the Curie-like 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 free-spin fraction generating Curie-like low-temperature χ is indeed expected in the RS picture12,20,21.

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 near-linear behavior expected for the RS state12, 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 field12,20. In general, there is a sharp change in the magnetization curve at the saturation field for non-randomness phase. By introducing bond-randomness, 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 near-linear 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 low-temperature regions below 0.5 K, a clear gapless T-linear behavior was observed, C p $$\simeq \,\gamma T$$. This T-linear behavior is robust against an applied magnetic field and appears even under a high-magnetic field near the saturation field. Such T-linear behavior of the specific heat is consistent with the specific heat expected in the RS picture21, 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 state3,6. We roughly evaluated γ from the C p/T values at the lowest temperatures and obtained 1.20 and 0.72 J/mol K2 at 0 and 3 T, respectively. From numerical analysis of the RS state, we thus deduced that the T-linear term of C p is strongly dependent on the fundamental ground state without randomness and, also, on the degree of introduced randomness12,20,21. The obtained γ-values 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 non-frustrated case) owing to strong quantum fluctuation27,28. From the theoretical analysis, it is deduced that the introduction of bond-randomness into the gapped phases is more effective for RS state formation than introduction into the gapless ordered phase12,20,21. Therefore, in the present model, the lattice distortion as well as the weak frustrated interaction should enhance the bond-randomness effect, inducing formation of the RS state.

In summary, we have succeeded in synthesizing single crystals of the verdazyl-based complex Zn(hfac)2(A x B1−x ). Two different regioisomers, A-type (x) and B-type (1-x), 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 liquid-like 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 liquid-like behavior. Furthermore, our method to introduce a bond-randomness into spin lattices enable further investigations on the randomness-induced QSL in other lattice systems.

## Methods

We synthesized Zn(hfac)2(A x B1−x ) using a conventional procedure similar to that used to prepare the typical verdazyl radical 1,3,5-triphenylverdazyl29. A solution of p-Cl-o-Py-V [1-(4-chlorophenyl)-3-(2-pyridyl)-5-phenylverdazyl] (119 mg, 0.34 mmol) in 10 ml of CH2Cl2 was slowly added to a solution of [Zn(hfac)2]·2H2O (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 dark-green crystalline solid of Zn(hfac)2(A x B1−x ) was separated by filtration and washed with pentane. The dark-green residue was recrystallized using CH2Cl2 in an acetonitrile atmosphere. The crystal structure was determined on the basis of intensity data collected using a Rigaku AFC-8R Mercury CCD RA-Micro7 diffractometer with a Japan Thermal Engineering XR-HR10K. The magnetizations were measured down to approximately 80 mK using a commercial SQUID magnetometer (MPMS-XL, 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 hand-made apparatus and a standard adiabatic heat-pulse 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 broken-symmetry hybrid-density 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 scheme30.

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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 joint-research program involving the Institute for Solid State Physics (ISSP), the University of Tokyo, and the Institute for Molecular Science.

## Author information

### Affiliations

1. #### Department of Physical Science, Osaka Prefecture University, Osaka, 599-8531, Japan

• Hironori Yamaguchi
• , Toshiki Okabe
• , Yoshiki Iwasaki
•  & Yuko Hosokoshi
2. #### Institute for Solid State Physics, The University of Tokyo, Chiba, 277-8581, Japan

• Yohei Kono
• , Shunichiro Kittaka
•  & Toshiro Sakakibara

### Contributions

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.

### Competing Interests

The authors declare that they have no competing interests.

### Corresponding author

Correspondence to Hironori Yamaguchi.