Abstract
The robustness of the macroscopic quantum nature of a superconductor can be characterized by the superfluid stiffness, ρs, a quantity that describes the energy required to vary the phase of the macroscopic quantum wavefunction. In unconventional superconductors, such as cuprates, the low-temperature behaviour of ρs markedly differs from that of conventional superconductors owing to quasiparticle excitations from gapless points (nodes) in momentum space. Intensive research on the recently discovered magic-angle twisted graphene family has revealed, in addition to superconducting states, strongly correlated electronic states associated with spontaneously broken symmetries, inviting the study of ρs to uncover the potentially unconventional nature of its superconductivity. Here we report the measurement of ρs in magic-angle twisted trilayer graphene (TTG), revealing unconventional nodal-gap superconductivity. Utilizing radio-frequency reflectometry techniques to measure the kinetic inductive response of superconducting TTG coupled to a microwave resonator, we find a linear temperature dependence of ρs at low temperatures and nonlinear Meissner effects in the current-bias dependence, both indicating nodal structures in the superconducting order parameter. Furthermore, the doping dependence shows a linear correlation between the zero-temperature ρs and the superconducting transition temperature Tc, reminiscent of Uemura’s relation in cuprates, suggesting phase-coherence-limited superconductivity. Our results provide strong evidence for nodal superconductivity in TTG and put strong constraints on the mechanisms of these graphene-based superconductors.
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Data availability
Source data are provided with the paper. All other data that support the findings of this study are available from the corresponding authors upon reasonable request.
Change history
07 April 2025
In the version of the article initially published, the grant no. NSF DMR-2220703 appeared incorrectly and has now been amended in the HTML and PDF versions of the article.
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Acknowledgements
We thank S. Kivelson and E. Berg for discussions. The major experimental work is supported by ARO MURI (W911NF-21-2-0147). P.K. and A.B. acknowledge support from the DOE (DE-SC0012260). M.K. is supported by the STC Center for Integrated Quantum Materials, NSF Grant number DMR-1231319. A.V., P.L. and P.A.V. are supported by a Simons Investigator grant (A.V.) and by NSF DMR-2220703. P.A.V. acknowledges support by a Quantum-CT Quantum Regional Partnership Investments (QRPI) Award. K.C.F. thanks M. Randeria for her musings inspiring this research direction. A.Y. and M.E.W. are supported by the Quantum Science Center (QSC), a National Quantum Information Science Research Center of the US Department of Energy (DOE). A.Y. is also partly supported by the Gordon and Betty Moore Foundation through grant GBMF ID #12762. K.W. and T.T. acknowledge support from the JSPS KAKENHI (grant numbers 21H05233 and 23H02052) and World Premier International Research Center Initiative (WPI), MEXT, Japan. Nanofabrication was performed at the Center for Nanoscale Systems at Harvard, supported in part by an NSF NNIN award ECS- 00335765.
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A.B., Z.H., M.K., K.C.F, and P.K. conceived of the experiment. Z.H., I.P., J.M.P. and A.Z. fabricated the devices, A.B., Z.H., M.E.W. and M.K. conducted the measurements and analysed the data. P.L., P.A.V. and A.V. conducted the theoretical analysis. R.M.W., A.Y., P.J.-H, P.A.V., A.V., K.C.F. and P.K. supervised the project. All authors discussed and wrote the paper. K.W. and T.T. supplied hBN crystals.
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Extended data figures and tables
Extended Data Fig. 1 Device DC transport characterization.
a, TTG 4-terminal R as a function of ν and magnetic field B at zero displacement field and a temperature of 2 K. The Landau fans show two set of structures: one set with large slopes and the other that appear at low B with shallow slopes. b, TTG 4-terminal R as a function of ν and displacement field D at zero B and a temperature of 30 mK.
Extended Data Fig. 2 Measurement setup.
Circuit model of measurement setup for superfluid stiffness measurements. The moiré graphene sample is indicated by dashed pink lines while the circuit board–containing sample, LC matching network, and bias tees to allow impedance matching for microwave measurement–is indicated by dashed purple lines. DC and RF filtering is used to reduce noise throughout the measurement chain. The RF signal is sent through an attenuated input line before entering a directional coupler. Sample contact resistance of ≃ 3.2 kΩ is given by Rc. Graphite top and bottom gates are represented by “gate”. The final signal is amplified both at 4 K and room temperature before being measured by a vector network analyzer (VNA).
Extended Data Fig. 3 Circle fitting.
(a) Circle fitting of S21 in the complex plane. (b) Fitting of the reflection amplitude ∣S21(f)∣. (c) Fitting of the phase expressed in degrees \(\arg {S}_{21}(f)\).
Extended Data Fig. 4 Uemura’s law.
Scaling of ρs0 versus Tc (obtained from resistance measurements) for both electron and hole side superconductors in all measured devices. A roughly linear trend is generally observed, even for devices with twist-angle disorder.
Extended Data Fig. 5 Superfluid stiffness in NbN thin films.
(a) Optical micrograph of a NbN thin film device with a meandering Au strip. The Au strip provides an additional resistance of 2.9 kΩ to mimic the contact resistance of TTG devices. We measured NbN samples thickness of 5 nm (NbN-5nm) and 8 nm (NbN-8nm) (b) Normalized superfluid stiffness ρs(T)/ρs0 as a function of temperature T normalized with respect to the superconducting transition temperature Tc for TTG and NbN devices. TTG shows monotonically rising stiffness as the temperature is lowered, with a linear behavior for T/Tc≤0.3. On the other hand, the NbN devices show a robust saturation of the stiffness for T/Tc≤0.3. The NbN stiffness data obeys the BCS expectation. The BCS fit is given by \({\rho }_{s}(T)/{\rho }_{s0}=\Delta (T)/{\Delta }_{0}\tanh (\Delta (T)/T)\) where \(\Delta (T)={\Delta }_{0}\tanh ({\rm{\pi }}{T}_{c}/{\Delta }_{0}\sqrt{{T}_{c}/T-1}),{\Delta }_{0}=1.76{k}_{B}{T}_{c}\).
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Banerjee, A., Hao, Z., Kreidel, M. et al. Superfluid stiffness of twisted trilayer graphene superconductors. Nature 638, 93–98 (2025). https://doi.org/10.1038/s41586-024-08444-3
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DOI: https://doi.org/10.1038/s41586-024-08444-3
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