Skip to main content

Thank you for visiting You are using a browser version with limited support for CSS. To obtain the best experience, we recommend you use a more up to date browser (or turn off compatibility mode in Internet Explorer). In the meantime, to ensure continued support, we are displaying the site without styles and JavaScript.

Pressure-tuning the quantum spin Hamiltonian of the triangular lattice antiferromagnet Cs2CuCl4


Quantum triangular-lattice antiferromagnets are important prototype systems to investigate numerous phenomena of the geometrical frustration in condensed matter. Apart from highly unusual magnetic properties, they possess a rich phase diagram (ranging from an unfrustrated square lattice to a quantum spin liquid), yet to be confirmed experimentally. One major obstacle in this area of research is the lack of materials with appropriate (ideally tuned) magnetic parameters. Using Cs2CuCl4 as a model system, we demonstrate an alternative approach, where, instead of the chemical composition, the spin Hamiltonian is altered by hydrostatic pressure. The approach combines high-pressure electron spin resonance and r.f. susceptibility measurements, allowing us not only to quasi-continuously tune the exchange parameters, but also to accurately monitor them. Our experiments indicate a substantial increase of the exchange coupling ratio from 0.3 to 0.42 at a pressure of 1.8 GPa, revealing a number of emergent field-induced phases.


The interplay between geometrical frustration, quantum fluctuations, and magnetic order is one of the central issues in condensed matter physics. In 1973, developing the resonating valence bond (RVB) theory, Anderson proposed that quantum fluctuations in magnetic structures on an isotropic triangular lattice can be sufficiently strong to destroy the magnetic order, resulting in a two-dimensional (2D) fluid of mobile spin pairs correlated together into singlets1. This state was introduced as a RVB quantum spin liquid, contrary to the valence-bond solid (VBS), with the ground state condensed into a spin lattice. The Anderson’s hypothesis has triggered a cascade of extensive theoretical and experimental studies, resulting in the discovery of numerous exotic quantum states and highly unusual field-induced phenomena2.

The spin-1/2 triangular-lattice Heisenberg antiferromagnet (AF) represents one of the most important groups of the family of low-D quantum frustrated magnets. For the general case of spatially anisotropic triangular AF, the spin Hamiltonian is given as

$${\cal H} = J\mathop {\sum}\limits_{\langle i,j\rangle } {\mathbf{S}}_i \cdot {\mathbf{S}}_j + J^{\prime}\mathop {\sum}\limits_{\langle i,j^{\prime}\rangle } {\mathbf{S}}_i \cdot {\mathbf{S}}_{j^{\prime}},$$

where Si, Sj, and Sj are spin-1/2 operators at sites i, j, and j′, and J and J′ are the exchange interactions on the horizontal and diagonal bonds, respectively (Fig. 1a, inset). In spite of this simple model, such systems are shown to possess a very rich and not fully understood phase diagram, which can be interpolated between decoupled spin-chain (J′ = 0), isotropic triangular (J′/J = 1), and unfrustrated square (J = 0) lattices. It is expected that transitions from one state to another occur in between these well-defined cases, but many details of this evolution (e.g., critical coupling ratios) still remain a matter of debate3,4. The magnetic phase diagram predicts a variety of exotic phases, with the 1/3 saturation-magnetization plateau as the most exciting magnetic property5.

Fig. 1

Pressure dependence of ESR excitations in Cs2CuCl4 (T = 1.9 K, H||b). a Frequency-field diagrams of ESR excitations at different pressures. The data denoted in black are taken from ref. 6 (T = 1.5 K; 0 GPa). Dashed lines correspond to the fit results (see text for details). Source data are provided as a Source Data file. The inset shows a schematic picture of magnetic sites and exchange couplings in a triangular layer of Cs2CuCl4. b ESR spectra (mode B) taken at 330 GHz at different pressures (the spectra are offset for clarity)

The largest hindrance to experimentally check theoretical predictions on the unusual magnetic properties of spin-1/2 triangular lattice Heisenberg AFs is the very limited number of materials with appropriate (ideally tuned) sets of parameters, currently available for measurements. In spite of the recent progress in synthesizing spin-1/2 triangular-lattice materials (see e.g., ref. 2 and references therein), the two compounds, Cs2CuCl4 and Cs2CuBr4 (with J′/J 0.30 and 0.41, respectively6), remain among the most prominent representatives of this family of frustrated materials. One obvious approach to tune the spin Hamiltonian of these systems is to vary their chemical composition7,8. However, experiments on the solid solution Cs2CuCl4−xBrx (with Br content ranging from 0 to 4) revealed a pronounced difference in the Cu coordination when increasing x, resulting in a discontinuous evolution of its crystal structure9.

The high-pressure technique is known as a powerful means to modify magnetic properties and parameters of exchange coupled spin systems (see e.g., refs. 10,11,12,13,14,15,16,17,18,19). On the other hand, another important task is to precisely measure these parameters. This becomes particularly challenging for low-D spin systems, whose spin Hamiltonian is strongly affected by quantum fluctuations. One solution to solve this problem is to suppress quantum fluctuations by strong-enough magnetic fields, and then to use the harmonic spin-wave theory for a description of the excitation spectrum6,20.

Here, we combine high-pressure high-field electron spin resonance (ESR) and radio frequency (r.f.) susceptibility measurements, allowing us not only to quasi-continuously change the exchange parameters J and J′, but also to accurately monitor them. We use Cs2CuCl4 as a model system. We show that the application of pressure increases significantly the exchange coupling parameters in this compound, triggering, at the same time, the emergence of field-induced low-temperature magnetic phases, absent at zero pressure.


High-pressure ESR measurements

To determine the dependence of the coupling parameters of Cs2CuCl4 on the applied pressure, we used the procedure employed in ref. 6, when the excitation spectrum is measured above the saturation field Hsat. In the case of the staggered Dzyaloshinskii–Moriya (DM) interaction, the ESR spectrum should consist of two modes, which correspond to magnetic excitations at the center and at the boundary of the unfolded Brillouin zone (a.k.a. the relativistic and exchange modes, respectively). Such modes were previously observed in Cs2CuCl46 (black symbols in Fig. 1a). The field dependence of the relativistic mode A for \(H \,\gtrsim \, J/g\mu _{\mathrm{B}}\) can be described using the equation ωA = BH, where is the reduced Planck constant, ω is the excitation frequency, μB is the Bohr magneton, and g = 2.06 is the g factor (the fit results are shown in Fig. 1a by the black dashed line). On the other hand, the frequency-field diagram of mode B can be described using the equation ωB = BH − ΔB (magenta dashed line in Fig. 1a) with the same g factor as for the mode A. Most importantly, the difference between the excitation energies for modes A and B (ΔωAB ≡ ΔB) is determined by J′: J′ = ΔωAB/4, allowing us to measure J′ directly. The experiment revealed a shift of the mode B towards higher field when the pressure is applied. The pressure dependence of J′ is shown in Fig. 2a, evident in a significant, almost 70%, increase of J′ at 1.92 GPa.

Fig. 2

Pressure-driven tuning of the spin-Hamiltonian parameters in Cs2CuCl4. a Pressure dependence of the exchange coupling parameters J′ and J (circles and boxes, respectively). The dashed line corresponds to a linear fit to the J′ data (see text for details).  b Pressure dependence of the exchange coupling ratio  J′/J. The dashed line corresponds to a linear fit to the J′/J data (see text for details). Source data are provided as a Source Data file

High-pressure TDO measurements

Knowing J′ and the saturation field Hsat, we can determine J, using the expression BHsat = 2J(1 + J′/2J)2. To measure the saturation field of Cs2CuCl4, we employ a tunnel-diode-oscillator (TDO) technique (see Methods). The variations of the TDO circuit resonant frequency Δf/f (which is proportional to the magnetic susceptibility) as a function of the magnetic field applied along the b axis at different pressures are shown in Fig. 3a. In strong magnetic fields, the TDO frequency is almost constant, indicating the transition of Cs2CuCl4 into the fully spin-polarized phase with saturated magnetization21. The experiment revealed that with increasing pressure the saturation field moves toward higher magnetic fields. The dependence of Hsat on the applied pressure is shown in Fig. 3b.

Fig. 3

Pressure evolution of magnetic properties of Cs2CuCl4 obtained by means of TDO technique (T = 350 mK, H||b). a Pressure dependence of the TDO frequency changes Δf/f in response to the magnetic field (the data are offset for clarity). b Dependencies of TDO frequency anomalies on the applied pressure. The calculated exchange coupling ratio J′/J is shown on the top scale (see text for details). Lines are guides for the eye. Source data are provided as a Source Data file

Based on the combined ESR and TDO data, for zero pressure we obtained J′/kB = 1.38 K and J/kB = 4.66 K (J′/J 0.3), which perfectly agrees with the previous estimates6. Results of a linear fit to the J′ dependence (dashed line in Fig. 2a) were used to calculate J at different pressures. J′, J, and J′/J as functions of the applied pressure are shown in Fig. 2. The J′/J dependence can be described using the empirical equation J′/J = 0.294(2) + 0.067(2)P (dashed line in Fig. 2b), where P is the applied pressure (GPa). For 1.8 GPa, we obtained J′/kB = 2.28 K, J/kB = 5.47 K, and J′/J 0.42, indicating a remarkable, by 40%, increase of the J′/J ratio. Based on this fit, the application of a pressure of 3.6 GPa (where Cs2CuCl4 undergoes a structural phase transition22) would allow one to reach \(J^{\prime}/J \simeq 0.53\) (which corresponds to approximately 180% of the zero-pressure value).


Apart from the shift of the saturation field, our experiment revealed a number of magnetic anomalies, which are absent in Cs2CuCl4 at zero pressure (Fig. 3a). The observed magnetic anomalies can be caused by changes in the dynamics of critical fluctuations in the vicinity of field-induced phase transitions23, resulting in changes of real and imaginary components of the magnetic susceptibility. Although no signature of the 1/3 magnetization plateau was revealed, our observation (Fig. 3b) resembles the cascade of field-induced phase transitions in quasi-2D Cs2CuBr424, evident of a complex picture of magnetic interactions, including different perturbation terms (a remarkable sensitivity of the magnetic phase diagrams of Cs2CuCl4 to the direction of the applied magnetic field21 strongly suggests an important role not only spatial (J′ ≠ J), but also spin-space (asymmetric DM interaction) components of the magnetic anisotropy; the latter appear to be of the same order of magnitude as the interplane exchange interaction J20, inducing strongly relevant perturbations25).

For the magnetic field applied along the b axis, the zero-pressure magnetic phase diagram contains four low-temperature phases21. At small field below TN = 0.62 K, the system is in the incommensurate phase with a spiral ground state26 dominantly determined by the DM anisotropy (“DM spiral”)25. In this phase, the spins are located almost in the bc plane with the spiral propagating along the b axis26. Remarkably, at about 2.3 T the effect of the DM interaction becomes irrelevant and the system undergoes a transition into the commensurate coplanar AF phase with spins more correlated in ab planes (the corresponding correlations are determined by J″ and J)25. These two magnetic phases are stabilized by quantum fluctuations. The commensurate coplanar AF state is realized in a relatively wide field range, followed by two successive high-field transitions: into the noncoplanar cone phase and then, with further increase of the applied magnetic field, into the fully spin-polarized magnetically saturated phase (both phases are favored classically).

What happens when pressure is applied? Apart from the shift of the saturation field, our experiment revealed a number of magnetic transitions, absent at zero pressure (Fig. 3a). The proposed magnetic phase diagram for 1.8 GPa is shown in Fig. 4. Similar to that at zero pressure, at low field the system is in the DM spiral phase. The DM spiral phase is suppressed by the magnetic field at about 2.2–2.6 T (the anomaly A in Fig. 3a corresponds to this transition), resulting in the commensurate coplanar AF phase with spins predominantly correlated in the ab plane. Applied pressure makes the J′ term more and more relevant, tending to suppress the coplanar nature of magnetic correlations. As a combined effect of the applied magnetic field (partially suppressing quantum order) and pressure (enhancing the interplane correlations), at about 6.9 T the system undergoes a transition into a noncoplanar (presumably) frustrated phase. The observed anomaly B corresponds to this transition.

Fig. 4

The proposed phase diagram of Cs2CuCl4 under pressure 1.8 GPa (which corresponds to J′/J = 0.42)

For a spatially anisotropic triangular lattice AF in magnetic fields near the saturation, theory27 predicts a particular rich phase diagram, with ground states ranging from an incommensurate noncoplanar chiral cone to a commensurate coplanar V state. The transformation between these two states involves two intermediate phases. One of them is a coplanar incommensurate order, while another one is a noncoplanar double-Q spiral order (double-cone state). The latter is characterized by the broken Z2 symmetry between two magnon condensates at ±Q (where Q is the ordering wave vector) and can coexist with the single-cone phase in a relatively narrow range of J′/J, but at smaller fields. In Cs2CuCl4 at zero pressure, the transition into the single-cone phase was revealed between 8 and 9 T below 300 mK21. Due to the increase of exchange coupling parameters, the applied pressure shifts the upper boundary of the temperature-field phase diagram to higher temperatures. Because of that, the transition into the single-cone phase can be observed at higher temperatures. Based on this assumption, the anomalies C and D (Fig. 3). can be interpreted as transitions into the double- and single-cone phases, respectively (Fig. 4). A tiny feature immediately before saturation might indicate the involvement of other higher-order perturbation factors (e.g., next-nearest-neighbor interactions28 or the interplane frustration mentioned above29).

Our observations call for systematic high-pressure magneto-structural (such as nuclear magnetic resonance and neutron diffraction) studies of Cs2CuCl4, which would allow one to verify the proposed phase diagram. Apart from exact identification of the nature of the observed high-pressure phases, another important task would be the search for the field-induced 1/3 magnetization plateau, which can be expected with further increase of J′/J moving the system towards the isotropic (J′/J = 1) limit27. It would be also very interesting to measure the pressure-driven evolution of the spin Hamiltonian in the isostructural compound Cs2CuBr4 and to compare the results with that in Cs2CuCl4.

To conclude, we demonstrated an effective strategy to control the spin Hamiltonian of a spin-1/2 antiferromagnet on a triangular lattice with hydrostatic pressure. With increasing pressure, for Cs2CuCl4 our experiments revealed a substantial increase of the exchange coupling parameters, accompanied by the emergence of (at least) two field-induced phases. These phases can be tentatively interpreted as noncoplanar frustrated and double-cone states, merging the low-field commensurate coplanar and high-field single-cone phases revealed previously. Our approach provides robust means for investigating the complex interplay between geometrical frustration, quantum fluctuations, and magnetic order (especially, close to quantum phase transitions), paving the way towards controlled manipulation of the spin Hamiltonian and magnetic properties of frustrated spin systems.


Single-crystal growth

Single-crystal samples of Cs2CuCl4 were grown by the slow evaporation of an aqueous solution of CsCl and CuCl2 in the mole ratio 2:1.

High-pressure TDO

High-pressure TDO measurements were conducted at the National High Magnetic Field Laboratory (Florida State University) in magnetic fields up to 18 T using a TDO susceptometer14,15,30 tuned to operate at a resonant frequency of 51 MHz. Magnetic field was applied along the b axis of the crystal. A sample with a length of ~1.5 mm was placed in a copper-wire coil with diameter ~0.8 mm and height ~1 mm. The coil and sample were surrounded with Daphne 7575 oil (Idemitsu Kosan Co., Ltd.) and encapsulated in a Teflon cup which was inserted into the bore of a piston-cylinder pressure cell constructed from a chromium alloy (MP35N). The coil acts as an inductor in a diode-biased self-resonant LC tank circuit. During the field sweep, changes in the sample magnetic permeability lead to changes in the inductance of the oscillator tank coil, and, hence, to changes in the TDO circuit resonant frequency Δf. The frequency changes were detected as a function of the magnetic field at different pressures. The pressure created in the cell was calibrated at room temperature and again at low temperature using the fluorescence of the R1 peak of a small ruby chip as a pressure marker31 with accuracy better than ±0.015 GPa. The pressure cell was immersed directly into 3He, allowing TDO measurements down to 350 mK. Temperature was measured using a calibrated Cernox thermometer. Transition fields were measured with accuracy better than ±0.5%.

High-pressure ESR

High-pressure ESR measurements of Cs2CuCl4 were performed at the High Field Laboratory for Superconducting Materials, Institute for Material Research (IMR), Tohoku University using a transmission-type ESR probe32,33 with oversized waveguides and a 25 T cryogen-free superconducting magnet34,35. Gunn-oscillators, operated at frequencies 220, 270, 330, and 405 GHz, were employed as radiation sources. A hot-electron InSb bolometer cooled down to 4.2 K was used as a detector. Magnetic field was applied along the b axis of the crystal. Experiments were performed at a temperature of 1.9(1) K; the temperature was measured using a calibrated Cernox thermometer. A cylinder-shaped crystal with approximate dimensions of 9 mm in length by 5 mm in diameter was immersed in a Teflon cup filled with Daphne 7474 oil (Idemitsu Kosan Co., Ltd.) as pressure medium. A two-section piston cylinder pressure cell made from NiCrAl (inner cylinder) and CuBe (outer sleeve) has been used. The key feature of the pressure cell is the inner pistons, made of ZrO2 ceramics; this material has low loss for electromagnetic radiation with frequency up to 800 GHz. The change of the superconducting transition temperature of tin was used to calibrate the applied pressure36; the transition temperature was detected by AC magnetic susceptibility measurements. Applied pressure was calculated using the relation between the load at room temperature and the pressure obtained at around 3 K32; the pressure calibration accuracy is better than ±0.05 GPa. ESR line position (mode B) was measured with accuracy better than ±0.2%. In our experiments, we assume that the accuracies estimating J′, J, and J′/J including all possible error sources, are better than ±1%, ±4%, and ±5%, respectively.

Data availability

The data that support the findings of this study are available from the corresponding author upon reasonable request. The source data underlying Figs. 1a, 2a, b, and 3b are provided as Source Data files.


  1. 1.

    Anderson, P. W. Resonating valence bonds: a new kind of insulator? Mater. Res. Bull. 8, 153–160 (1973).

    CAS  Article  Google Scholar 

  2. 2.

    Balents, L. Spin liquids in frustrated magnets. Nature 464, 199–208 (2010).

    ADS  CAS  Article  Google Scholar 

  3. 3.

    Starykh, O. A. Unusual ordered phases of highly frustrated magnets: a review. Rep. Prog. Phys. 78, 052502 (2015).

    ADS  Article  Google Scholar 

  4. 4.

    Chen, R., Ju, H., Jiang, H.-C., Starykh, O. A. & Balents, L. Ground states of spin-1/2 triangular antiferromagnets in a magnetic field. Phys. Rev. B 87, 165123 (2013).

    ADS  Article  Google Scholar 

  5. 5.

    Ono, T. et al. Magnetization plateaux of the S = 1/2 two-dimensional frustrated antiferromagnet Cs2CuBr4. J. Phys. Condens. Matter 16, S773–S778 (2004).

    CAS  Article  Google Scholar 

  6. 6.

    Zvyagin, S. A. et al. Direct determination of exchange parameters in Cs2CuBr4 and Cs2CuCl4: high-field electron-spin-resonance studies. Phys. Rev. Lett. 112, 077206 (2014).

    ADS  CAS  Article  Google Scholar 

  7. 7.

    Ono, T. et al. Phase transitions and disorder effects in pure and doped frustrated quantum antiferromagnet Cs2CuBr4. J. Phys. Soc. Jpn. 74, 135–144 (2005).

    Article  Google Scholar 

  8. 8.

    van Well, N. et al. Magnetic phase diagram of the triangular antiferromagnetic Cs2CuCl4−xBrx mixed system. Ann. Phys. 530, 1800270 (2018).

    Article  Google Scholar 

  9. 9.

    Cong, P. T. et al. Distinct magnetic regimes through site-selective atom substitution in the frustrated quantum antiferromagnet Cs2CuCl4-xBrx. Phys. Rev. B 83, 064425 (2011).

    ADS  Article  Google Scholar 

  10. 10.

    Zaliznyak, I. A., Dender, D. C., Broholm, C. & Reich, D. H. Tuning the spin Hamiltonian of Ni(C2H8N2)2NO2ClO4 by external pressure: a neutron-scattering study. Phys. Rev. B 57, 5200–5204 (1998).

    ADS  CAS  Article  Google Scholar 

  11. 11.

    Goto, K., Fujisawa, M., Ono, T., Tanaka, H. & Uwatoko, Y. Pressure-induced magnetic quantum phase transition from gapped ground state in TlCuCl3. J. Phys. Soc. Jpn. 73, 3254–3257 (2004).

    ADS  CAS  Article  Google Scholar 

  12. 12.

    Rüegg, Ch. et al. Pressure-induced quantum phase transition in the spin-liquid TlCuCl3. Phys. Rev. Lett. 93, 257201 (2004).

    ADS  Article  Google Scholar 

  13. 13.

    Hong, T. et al. Effect of pressure on the quantum spin ladder material IPA-CuCl3. Phys. Rev. B 78, 224409 (2008).

    ADS  Article  Google Scholar 

  14. 14.

    Ghannadzadeh, S. et al. Evolution of magnetic interactions in a pressure-induced Jahn–Teller driven magnetic dimensionality switch. Phys. Rev. B 87(R), 241102 (2013).

    ADS  Article  Google Scholar 

  15. 15.

    Haravifard, S. et al. Crystallization of spin superlattices with pressure and field in the layered magnet SrCu2(BO3)2. Nat. Commun. 7, 11956 (2017).

    ADS  Article  Google Scholar 

  16. 16.

    Thirunavukkuarasu, K. et al. Pressure dependence of the exchange anisotropy in an organic ferromagnet. Phys. Rev. B 91, 014412 (2015).

    ADS  Article  Google Scholar 

  17. 17.

    Zayed, M. E. et al. 4-spin plaquette singlet state in the Shastry–Sutherland compound SrCu2(BO3)2. Nat. Phys. 13, 962–966 (2017).

    MathSciNet  CAS  Article  Google Scholar 

  18. 18.

    Skoulatos, M. et al. Dimensional reduction by pressure in the magnetic framework material CuF2(D2O)2(pyz): from spin-wave to spinon excitations. Phys. Rev. B 96, 020414 (2017).

    ADS  Article  Google Scholar 

  19. 19.

    Wehinger, B. et al. Giant pressure dependence and dimensionality switching in a metal–organic quantum antiferromagnet. Phys. Rev. Lett. 121, 117201 (2018).

    ADS  CAS  Article  Google Scholar 

  20. 20.

    Coldea, R. et al. Direct measurement of the spin Hamiltonian and observation of condensation of magnons in the 2D frustrated quantum magnet Cs2CuCl4. Phys. Rev. Lett. 88, 137203 (2002).

    ADS  CAS  Article  Google Scholar 

  21. 21.

    Tokiwa, Y. et al. Magnetic phase transitions in the two-dimensional frustrated quantum antiferromagnet Cs2CuCl4. Phys. Rev. B 73, 134414 (2006).

    ADS  Article  Google Scholar 

  22. 22.

    Xu, Y., Söderberg, C. K. & Norrestam, R. High-pressure studies of Cs2CuCl4 and Cs2CoCl4 by X-ray diffraction methods. J. Solid State Chem. 153, 212–217 (2000).

    ADS  CAS  Article  Google Scholar 

  23. 23.

    Kawasaki, K. Kinetic equations and time correlation functions of critical fluctuations. Ann. Phys. 61, 1–56 (1970).

    ADS  CAS  Article  Google Scholar 

  24. 24.

    Fortune, N. A. et al. Cascade of magnetic-field-induced quantum phase transitions in a spin-1/2 triangular-lattice antiferromagnet. Phys. Rev. Lett. 102, 257201 (2009).

    ADS  CAS  Article  Google Scholar 

  25. 25.

    Starykh, O. A., Katsura, H. & Balents, L. Extreme sensitivity of a frustrated quantum magnet: Cs2CuCl4. Phys. Rev. B 82, 014421 (2010).

    ADS  Article  Google Scholar 

  26. 26.

    Coldea, R. et al. Neutron scattering study of the magnetic structure of Cs2CuCl4. J. Phys. Condens. Matter 8, 7473–7491 (1996).

    ADS  CAS  Article  Google Scholar 

  27. 27.

    Starykh, O. A., Jin, W. & Chubukov, A. V. Phases of a triangular-lattice antiferromagnet near saturation. Phys. Rev. Lett. 113, 087204 (2014).

    ADS  Article  Google Scholar 

  28. 28.

    Ye, M. & Chubukov, A. V. Half-magnetization plateau in a Heisenberg antiferromagnet on a triangular lattice. Phys. Rev. B 96, 140406(R) (2017).

    ADS  Article  Google Scholar 

  29. 29.

    Stone, M. B. et al. Singlet-triplet dispersion reveals additional frustration in the triangular-lattice dimer compound Ba3Mn2O8. Phys. Rev. Lett. 100, 237201 (2008).

    ADS  CAS  Article  Google Scholar 

  30. 30.

    Clover, R. B. & Wolf, W. P. Magnetic susceptibility measurements with a tunnel diode oscillator. Rev. Sci. Instrum. 41, 617–621 (1970).

    ADS  CAS  Article  Google Scholar 

  31. 31.

    Piermarini, G. J., Block, S., Barnett, J. D. & Forma, R. A. Calibration of the pressure dependence of the R1 ruby fluorescence line to 195 kbar. J. Appl. Phys. 46, 2774–2780 (1975).

    ADS  CAS  Article  Google Scholar 

  32. 32.

    Sakurai, T. et al. Development of multi-frequency ESR system for high-pressure measurements up to 2.5 GPa. J. Magn. Reson. 259, 108–113 (2015).

    ADS  CAS  Article  Google Scholar 

  33. 33.

    Sakurai, T. et al. Direct observation of the quantum phase transition of SrCu2(BO3)2 by high-pressure and terahertz electron spin resonance. J. Phys. Soc. Jpn. 87, 033701 (2018).

    ADS  Article  Google Scholar 

  34. 34.

    Awaji, S. et al. First performance test of a 25 T cryogen-free superconducting magnet. Supercond. Sci. Technol. 30, 065001 (2017).

    ADS  Article  Google Scholar 

  35. 35.

    Sakurai, T. et al. Development and application of 2.5 gigapascal-25 Tesla high-pressure high-field electron spin resonance system using a cryogen-free superconducting magnet. J. Magn. Reson. 296, 1–4 (2018).

    ADS  CAS  Article  Google Scholar 

  36. 36.

    Smith, T. F. et al. Will pressure destroy superconductivity? Phys. Rev. 159, 353–358 (1967).

    ADS  CAS  Article  Google Scholar 

Download references


This work was partially supported by Deutsche Forschungsgemeinschaft through the projects ZV6/2-2, SFB 1143, and the Würzburg-Dresden Cluster of Excellence on Complexity and Topology in Quantum Matter - ct.qmat (EXC 2147, project-id39085490). We acknowledge support by the HLD at HZDR, member of the European Magnetic Field Laboratory (EMFL). A portion of this work was performed at the National High Magnetic Field Laboratory, which is supported by the National Science Foundation Cooperative Agreement No. DMR-1644779 and the State of Florida. ESR experiments were performed at the High Field Laboratory for Superconducting Materials, Institute for Material Research, Tohoku University (proposals 18H0059 and 17H0071). H.N. acknowledges the support of the KAKENHI 16H04005 Program. S.A.Z. acknowledges the support of the ICC-IMR Visitor Program at Tohoku University. The authors would like to thank O.A. Starykh, R. Valentí, C.D. Batista, L. Balents, and R. Coldea for fruitful discussions, and A. Ponomaryov for the help orienting the samples.

Author information




S.A.Z. conceived, designed, and led the project. T.O. and H.T. grew Cs2CuCl4 single crystals. D.G. and S.A.Z. performed high-field magnetization experiments. T.S., S.K., H.N., and S.A.Z. performed high-field ESR experiments. J.W. and H.O. administered the HLD and KU parts of the project, respectively. All authors discussed the results and commented on the manuscript.

Corresponding author

Correspondence to S. A. Zvyagin.

Ethics declarations

Competing interests

The authors declare no competing interests.

Additional information

Journal peer review information: Nature Communications thanks D.A. Tennant and the other anonymous reviewers for their contribution to the peer review of this work.

Publisher’s note: Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Supplementary data

Rights and permissions

Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit

Reprints and Permissions

About this article

Verify currency and authenticity via CrossMark

Cite this article

Zvyagin, S.A., Graf, D., Sakurai, T. et al. Pressure-tuning the quantum spin Hamiltonian of the triangular lattice antiferromagnet Cs2CuCl4. Nat Commun 10, 1064 (2019).

Download citation

Further reading


By submitting a comment you agree to abide by our Terms and Community Guidelines. If you find something abusive or that does not comply with our terms or guidelines please flag it as inappropriate.


Quick links

Nature Briefing

Sign up for the Nature Briefing newsletter — what matters in science, free to your inbox daily.

Get the most important science stories of the day, free in your inbox. Sign up for Nature Briefing