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Probing the quantum metric of 3D topological insulators

Abstract

The surface states of three-dimensional topological insulators possess geometric structures that imprint distinctive signatures on electronic transport. A prime example is the Berry curvature, which controls, for instance, electric frequency doubling via its higher-order moments. In addition to the Berry curvature, topological surface states are expected to exhibit a quantum metric, which plays a key role in nonlinear magnetotransport. Here we provide evidence for a nonlinear response activated by the quantum metric of the topological surface states of Sb2Te3. We measure a time-reversal-odd, nonlinear magnetoresistance that is independent of temperature and scattering time below 30 K, and is thus of intrinsic geometrical origin. This quantum metric magnetoresistance can be controlled by tuning the contributions of the top and bottom topological surface states through voltage gating. Our measurements demonstrate the existence and tunability of quantum geometry-induced transport in topological phases of matter and enable the design of functional topological devices.

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Fig. 1: Quantum geometry of a 3D topological insulator.
The alternative text for this image may have been generated using AI.
Fig. 2: Sb2Te3 topological insulator.
The alternative text for this image may have been generated using AI.
Fig. 3: Nonlinear magnetotransport.
The alternative text for this image may have been generated using AI.
Fig. 4: Quantum-metric-driven nonlinear conductivity.
The alternative text for this image may have been generated using AI.
Fig. 5: Gate voltage control of linear and nonlinear transport in Sb2Te3.
The alternative text for this image may have been generated using AI.

Data availability

The data that support the findings of this study are available via Zenodo at https://doi.org/10.5281/zenodo.16910820 (ref. 66) and from the corresponding authors upon reasonable request.

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Acknowledgements

We thank J.-M. Triscone for fruitful discussions and M. Lopes for technical support. We thank A. Morpurgo and I. Gutiérrez for support with the device fabrication. G.S. acknowledges support from the Swiss National Science Foundation (grant no. PZ00P2_223542). E.L. acknowledges the financial support from project nos. PID2023-152225NB-I00 and Severo Ochoa MATRANS42 (no. CEX2023-001263-S) of the Spanish Ministry of Science and Innovation (grant no. MICIU/AEI/10.13039/501100011033 and FEDER, EU), project nos. TED2021-129857B-I00 and PDC2023-145824-I00 funded by MCIN/AEI/10.13039/501100011033 and European Union NextGeneration EU/PRTR and by project no. 2021 SGR 00445 by the Generalitat de Catalunya. M.C. acknowledges support from the PNRR MUR project PE0000023-NQSTI and by the Italian Ministry of University and Research (MUR) PRIN 2022 under the grant no. 2022LP5K7 (BEAT). R.M. acknowledges the financial support from the PNRR MUR project PE0000023-NQSTI and the SPIGA project funded by the European Union – NextGeneration EU – PNRR – M4C2, Investment Line 1.1 – PRIN 2022 – ID P2022LXNYN. M.T.M. and C.O. acknowledge partial support by the Italian Ministry of Foreign Affairs and International Cooperation PGR12351 (ULTRAQMAT) and from PNRR MUR project no. PE0000023-NQSTI (TOPQIN). This work was supported by the Swiss State Secretariat for Education, Research and Innovation (SERI) under contract no. MB22.00071, by the Gordon and Betty Moore Foundation (grant no. 332 GBMF10451 to A.D.C.), by the European Research Council (ERC).

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Contributions

E.L. proposed the use of the Sb2Te3 topological insulator to probe the quantum metric. R.M. coordinated the production of Sb2Te3. G.S. and E.L. fabricated the devices, performed the transport measurements and data analysis with a contribution by S.G. The theory calculations were performed by M.T.M. with help from M.C. and C.O. The experimental work was supervised by A.D.C., and the theoretical work was supervised by C.O. All authors contributed to writing the paper with a first presentation provided by G.S.

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Correspondence to Giacomo Sala, Emanuele Longo, Carmine Ortix or Andrea D. Caviglia.

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Nature Materials thanks Su-Yang Xu and the other, anonymous, reviewer(s) for their contribution to the peer review of this work. Peer reviewer reports are available.

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Extended data

Extended Data Fig. 1 Linear transport.

a, Temperature dependence of the resistivity of Sb2Te3(30 nm) showing a metallic behavior. b, Temperature dependence of the total hole carrier density p and hole mobility μ estimated from measurements of the ordinary Hall effect.

Extended Data Fig. 2 Current dependence of the linear and nonlinear magnetoresistances.

a, Linear magnetoresistance measured at 10 K at increasing current with the field applied in the sample plane and perpendicular to the current direction. b, Nonlinear magnetoresistance measured simultaneously to the linear magnetoresistance in a. c Two-probe linear I-V curve demonstrating ohmic contacts.

Extended Data Fig. 3 Frequency dependence of the linear and nonlinear magnetoresistances.

Frequency dependence of the linear a and nonlinear b magnetoresistances measured at 10 K with a 500 μA current. The magnetic field was applied in the sample plane and perpendicular to the current direction.

Extended Data Fig. 4 Temperature dependence of the nonlinear magnetoresistance.

Temperature dependence of the nonlinear magnetoresistance at several magnetic fields and at gate voltages Vg = 0 V and Vg = −40 V in a and b, respectively.

Extended Data Fig. 5 Quantum-metric nonlinear conductivity as a function of the electronic mobility.

Quantum-metric nonlinear conductivity as a function of the electronic mobility at selected magnetic fields and at gate voltages Vg = 0 V and Vg = −40 V in a and b, respectively. The graphs on the right are a zoom-in on the high-mobility range, which corresponds to temperatures between 2 and 20 K.

Extended Data Fig. 6 Dependence of the linear and nonlinear magnetoresistances on the top-gate voltage.

a,b, Linear and nonlinear magnetoresistances, respectively, measured with an in-plane magnetic field oriented orthogonal to the current direction as a function of the top-electrode voltage, at a temperature T = 2.5 K and with an electric current Iω = 400 μA.

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Sala, G., Longo, E., Mercaldo, M.T. et al. Probing the quantum metric of 3D topological insulators. Nat. Mater. (2026). https://doi.org/10.1038/s41563-026-02617-3

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