Gate-tunable Josephson diodes in magic-angle twisted bilayer graphene
Pith reviewed 2026-05-18 06:32 UTC · model grok-4.3
The pith
Gate voltage can tune and reverse the polarity of Josephson diodes in magic-angle twisted bilayer graphene at fixed magnetic fields.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The central discovery is that the nonreciprocal supercurrent in these junctions arises from large kinetic inductance combined with non-uniform supercurrent distribution shaped by microscopic inhomogeneities such as twist angle variations. This leads to gate-tunable diode efficiency and the ability to reverse diode polarity at fixed magnetic fields, with adjacent junctions showing different interference patterns as a result of their local environments.
What carries the argument
The gate-tunable Josephson diode effect produced by large kinetic inductance and non-uniform supercurrent distribution due to twist angle inhomogeneities
If this is right
- The nonreciprocal supercurrent can be tuned by gate voltage.
- Diode efficiency can be adjusted and polarity reversed at fixed magnetic fields.
- Adjacent junctions show different diode behavior due to local microscopic inhomogeneities.
- This provides potential routes for tailoring Josephson diode performance in superconducting quantum circuits.
Where Pith is reading between the lines
- Electrically controllable Josephson diodes could be useful in quantum circuits where applying local magnetic fields is impractical.
- The findings may generalize to other two-dimensional superconducting systems with strong kinetic inductance and moiré patterns.
- Varying the gate to change carrier density could serve as a test to modulate the kinetic inductance and confirm its role in the diode effect.
Load-bearing premise
Microscopic inhomogeneities such as twist angle variations primarily shape the non-uniform supercurrent and drive the diode behavior rather than junction geometry or other disorder effects.
What would settle it
If the supercurrent distribution were found to be uniform across the junction or if the diode polarity showed no dependence on gate voltage while the magnetic field is held constant, the explanation based on inhomogeneities and kinetic inductance would be ruled out.
Figures
read the original abstract
We report low-temperature measurements of two adjacent, gate-defined Josephson junctions (JJs) in magic-angle twisted bilayer graphene (MATBG) at a moir\'e filling factor near $\nu = -2$. We show that both junctions exhibit a prominent, gate-tunable Josephson diode effect, which we explain by a combination of large kinetic inductance and non-uniform supercurrent distribution. Despite their proximity, the JJs display differences in their interference patterns and different diode behavior, underscoring that microscopic inhomogeneities such as twist angle variations shape the non-uniform supercurrent and drive the diode behavior. As a result, the nonreciprocal supercurrent can be tuned by gate voltage, enabling tuning of the diode efficiency and even reversing the polarity at fixed magnetic fields. Our findings offer potential routes for tailoring Josephson diode performance in superconducting quantum circuits.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports low-temperature transport measurements on two adjacent, gate-defined Josephson junctions fabricated in magic-angle twisted bilayer graphene near moiré filling factor ν = −2. Both junctions exhibit a prominent Josephson diode effect whose efficiency and polarity can be tuned by gate voltage, including polarity reversal at fixed magnetic field. The authors attribute the diode behavior to the combination of large kinetic inductance and a non-uniform supercurrent distribution, with the latter ascribed to microscopic inhomogeneities such as twist-angle variations; this interpretation is supported by observed differences in Fraunhofer interference patterns between the two nearby junctions.
Significance. If the proposed mechanism is substantiated, the work is significant because it demonstrates gate-tunable nonreciprocity in a highly tunable moiré superconductor and identifies inhomogeneity as a controllable ingredient for Josephson diode performance. The experimental observation of polarity reversal and differing diode characteristics in adjacent junctions constitutes a concrete advance for superconducting quantum-circuit applications. The authors receive credit for the clear experimental demonstration of gate control over the diode effect.
major comments (2)
- [Abstract / diode-effect explanation] Abstract and the paragraph explaining the diode effect: the central claim that twist-angle variations produce the non-uniform supercurrent distribution (and thereby the gate-tunable diode behavior) is load-bearing yet rests only on differences in interference patterns between the two junctions. No quantitative modeling of the expected supercurrent profile from measured or simulated twist-angle maps is provided, nor is a comparison made against alternative inhomogeneity sources such as strain, dielectric disorder, or edge scattering. This leaves the proposed mechanism for gate control and polarity reversal without direct experimental support.
- [Model / data comparison] Section describing the kinetic-inductance plus non-uniform-current model: the manuscript invokes standard kinetic-inductance concepts but does not show explicit calculations or fits that quantitatively reproduce the measured diode efficiency, its gate dependence, or the observed polarity reversal. Without such modeling, it is unclear whether the combination of large kinetic inductance and inhomogeneity accounts for the data or whether additional factors are required.
minor comments (1)
- [Figures] Figure captions and axis labels should explicitly state the range of gate voltages and magnetic fields over which the diode efficiency and polarity reversal are demonstrated, to allow readers to assess the tuning range directly.
Simulated Author's Rebuttal
We thank the referee for their thorough review and positive evaluation of our work. We address each major comment below and have made revisions to the manuscript to strengthen the presentation of our results and interpretations.
read point-by-point responses
-
Referee: [Abstract / diode-effect explanation] Abstract and the paragraph explaining the diode effect: the central claim that twist-angle variations produce the non-uniform supercurrent distribution (and thereby the gate-tunable diode behavior) is load-bearing yet rests only on differences in interference patterns between the two junctions. No quantitative modeling of the expected supercurrent profile from measured or simulated twist-angle maps is provided, nor is a comparison made against alternative inhomogeneity sources such as strain, dielectric disorder, or edge scattering. This leaves the proposed mechanism for gate control and polarity reversal without direct experimental support.
Authors: We agree that a more quantitative link between the observed differences in Fraunhofer patterns and specific inhomogeneity sources would strengthen the manuscript. The differing interference patterns in the two adjacent junctions, which are fabricated in close proximity, provide strong evidence for local microscopic variations. In the revised version, we have expanded the discussion to include a qualitative comparison of how twist-angle variations would affect the supercurrent distribution compared to strain or dielectric disorder, based on known sensitivities in MATBG. We note that direct twist-angle mapping via STM or similar techniques was not performed in this study, but the gate-tunability and polarity reversal are consistent with changes in the kinetic inductance interacting with a fixed non-uniform profile. We have added this clarification to the abstract and main text. revision: partial
-
Referee: [Model / data comparison] Section describing the kinetic-inductance plus non-uniform-current model: the manuscript invokes standard kinetic-inductance concepts but does not show explicit calculations or fits that quantitatively reproduce the measured diode efficiency, its gate dependence, or the observed polarity reversal. Without such modeling, it is unclear whether the combination of large kinetic inductance and inhomogeneity accounts for the data or whether additional factors are required.
Authors: We thank the referee for pointing this out. In the revised manuscript, we have added explicit calculations in the main text and supplementary information. Using a simple model of kinetic inductance combined with a non-uniform supercurrent distribution (parameterized by an asymmetry factor), we show that the diode efficiency η = (I_c^+ - I_c^-)/(I_c^+ + I_c^-) can reach values up to 0.3-0.5 for realistic kinetic inductance values in MATBG, and that gate-dependent changes in the inductance can lead to polarity reversal at fixed B field. These calculations qualitatively reproduce the observed gate dependence and the differences between the two junctions. We have included fits to the data where possible. revision: yes
Circularity Check
No circularity: experimental observations explained via standard concepts
full rationale
This is an experimental report on gate-tunable Josephson diodes in MATBG. The explanation invokes large kinetic inductance combined with non-uniform supercurrent distribution, inferred from measured differences in interference patterns between adjacent junctions. No equations, derivations, or fitted parameters are presented that reduce by construction to the inputs. No self-citation chains or ansatzes are load-bearing for the central claim. The attribution to twist-angle inhomogeneities is an interpretive inference from proximity and pattern differences rather than a self-referential definition or renaming. The paper remains self-contained against external benchmarks of Josephson junction physics.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Standard assumptions of Josephson junction physics and kinetic inductance in graphene-based superconductors hold without additional corrections.
Reference graph
Works this paper leans on
-
[1]
04 V) and right at others ( VR = 0 . 97 V, VR = 1 . 1 V). Furthermore, the prominence of the central oscillation increases at VR = 1. 055 V and VR = 1. 1 V. 5 We quantify the JD effect by first extracting the skew- ness of the interference patterns ( δB, defined as the dif- ference in supercurrent maxima between positive and negative bias within the central ...
-
[2]
2 mT. (b) Diode efficiency as a function of magnetic field extracted from the interference pattern taken at VL = 1. 06 V and VR = 1 . 01 V in Fig. 3. The shaded areas correspond to the errors arising from the fitting procedure. (c) Diode efficiency ηj extracted from measurements at constant mag- netic field values of B = 0 . 45 mT and B = − 0. 95 mT for the junc...
-
[3]
76kBTc is the supercon- ducting gap
7 K is the critical temperature, L, W are the length and width of the superconducting region, respectively, h is Planck’s constant, kB is the Boltzmann constant, R□ is the sheet resistance and ∆ ≈ 1. 76kBTc is the supercon- ducting gap. In our case, L and W roughly correspond to the length of a twist angle domain and to the penetration depth, respectively...
- [4]
-
[5]
F. Ando, Y. Miyasaka, T. Li, J. Ishizuka, T. Arakawa, Y. Shiota, T. Moriyama, Y. Yanase, and T. Ono, Obser- vation of superconducting diode effect, Nature 584, 373 (2020)
work page 2020
-
[6]
Y. Miyasaka, R. Kawarazaki, H. Narita, F. Ando, Y. Ikeda, R. Hisatomi, A. Daido, Y. Shiota, T. Moriyama, Y. Yanase, and T. Ono, Observation of nonreciprocal superconducting critical field, Appl. Phys. Express 14, 073003 (2021)
work page 2021
-
[7]
R. Kawarazaki, H. Narita, Y. Miyasaka, Y. Ikeda, R. Hisatomi, A. Daido, Y. Shiota, T. Moriyama, Y. Yanase, A. V. Ognev, A. S. Samardak, and T. Ono, Magnetic-field-induced polarity oscillation of supercon- ducting diode effect, Appl. Phys. Express 15, 113001 (2022)
work page 2022
-
[8]
Y. M. Itahashi, T. Ideue, Y. Saito, S. Shimizu, T. Ouchi, T. Nojima, and Y. Iwasa, Nonreciprocal transport in gate-induced polar superconductor SrTiO 3, Sci. Adv. 6, eaay9120 (2020)
work page 2020
-
[9]
T. Schumann, L. Galletti, H. Jeong, K. Ahadi, W. M. Strickland, S. Salmani-Rezaie, and S. Stemmer, Possible signatures of mixed-parity superconductivity in doped polar SrTiO 3 films, Phys. Rev. B 101, 100503 (2020)
work page 2020
-
[10]
R. Wakatsuki, Y. Saito, S. Hoshino, Y. M. Itahashi, T. Ideue, M. Ezawa, Y. Iwasa, and N. Nagaosa, Nonre- ciprocal charge transport in noncentrosymmetric super- conductors, Sci. Adv. 3, e1602390 (2017). 9
work page 2017
-
[11]
J.-X. Lin, P. Siriviboon, H. D. Scammell, S. Liu, D. Rhodes, K. Watanabe, T. Taniguchi, J. Hone, M. S. Scheurer, and J. I. A. Li, Zero-field superconducting diode effect in small-twist-angle trilayer graphene, Nat. Phys. 18, 1221 (2022)
work page 2022
-
[12]
H. D. Scammell, J. I. A. Li, and M. S. Scheurer, Theory of zero-field superconducting diode effect in twisted trilayer graphene, 2D Mater. 9, 025027 (2022)
work page 2022
-
[13]
H. Narita, J. Ishizuka, R. Kawarazaki, D. Kan, Y. Sh- iota, T. Moriyama, Y. Shimakawa, A. V. Ognev, A. S. Samardak, Y. Yanase, and T. Ono, Field-free supercon- ducting diode effect in noncentrosymmetric superconduc- tor/ferromagnet multilayers, Nat. Nanotechnol. 17, 823 (2022)
work page 2022
-
[14]
C. Baumgartner, L. Fuchs, A. Costa, S. Reinhardt, S. Gronin, G. C. Gardner, T. Lindemann, M. J. Manfra, P. E. Faria Junior, D. Kochan, J. Fabian, N. Paradiso, and C. Strunk, Supercurrent rectification and magne- tochiral effects in symmetric Josephson junctions, Nat. Nanotechnol. 17, 39 (2022)
work page 2022
-
[15]
K.-R. Jeon, J.-K. Kim, J. Yoon, J.-C. Jeon, H. Han, A. Cottet, T. Kontos, and S. S. P. Parkin, Zero-field polarity-reversible Josephson supercurrent diodes en- abled by a proximity-magnetized Pt barrier, Nat. Mater. 21, 1008 (2022)
work page 2022
-
[16]
H. Wu, Y. Wang, Y. Xu, P. K. Sivakumar, C. Pasco, U. Filippozzi, S. S. P. Parkin, Y.-J. Zeng, T. McQueen, and M. N. Ali, The field-free Josephson diode in a van der Waals heterostructure, Nature 604, 653 (2022)
work page 2022
-
[17]
B. Pal, A. Chakraborty, P. K. Sivakumar, M. Davydova, A. K. Gopi, A. K. Pandeya, J. A. Krieger, Y. Zhang, M. Date, S. Ju, N. Yuan, N. B. M. Schr¨ oter, L. Fu, and S. S. P. Parkin, Josephson diode effect from Cooper pair momentum in a topological semimetal, Nat. Phys. 18, 1228 (2022)
work page 2022
-
[18]
L. Bauriedl, C. B¨ auml, L. Fuchs, C. Baumgartner, N. Paulik, J. M. Bauer, K.-Q. Lin, J. M. Lupton, T. Taniguchi, K. Watanabe, C. Strunk, and N. Paradiso, Supercurrent diode effect and magnetochiral anisotropy in few-layer NbSe 2, Nat. Commun. 13, 4266 (2022)
work page 2022
-
[19]
J. D ´ ıez-M´ erida, A. D ´ ıez-Carl´ on, S. Y. Yang, Y.-M. Xie, X.-J. Gao, J. Senior, K. Watanabe, T. Taniguchi, X. Lu, A. P. Higginbotham, K. T. Law, and D. K. Efetov, Symmetry-broken Josephson junctions and supercon- ducting diodes in magic-angle twisted bilayer graphene, Nat. Commun. 14, 2396 (2023)
work page 2023
-
[20]
P. Chen, G. Wang, B. Ye, J. Wang, L. Zhou, Z. Tang, L. Wang, J. Wang, W. Zhang, J. Mei, W. Chen, and H. He, Edelstein Effect Induced Superconducting Diode Effect in Inversion Symmetry Breaking MoTe 2 Josephson Junctions, Adv. Funct. Mater. 34, 2311229 (2024)
work page 2024
-
[21]
A. Kudriashov, X. Zhou, R. A. Hovhannisyan, A. S. Frolov, L. Elesin, Y. B. Wang, E. V. Zharkova, T. Taniguchi, K. Watanabe, Z. Liu, K. S. Novoselov, L. V. Yashina, X. Zhou, and D. A. Bandurin, Non- Majorana origin of anomalous current-phase relation and Josephson diode effect in Bi2Se3/NbSe2 Josephson junc- tions, Sci. Adv. 11, 10.1126/sciadv.adw6925 (2025)
-
[22]
Y. Cao, V. Fatemi, S. Fang, K. Watanabe, T. Taniguchi, E. Kaxiras, and P. Jarillo-Herrero, Unconventional super- conductivity in magic-angle graphene superlattices, Na- ture 556, 43 (2018)
work page 2018
- [23]
-
[24]
J. M. Park, Y. Cao, K. Watanabe, T. Taniguchi, and P. Jarillo-Herrero, Tunable strongly coupled supercon- ductivity in magic-angle twisted trilayer graphene, Na- ture 590, 249 (2021)
work page 2021
-
[25]
J. M. Park, Y. Cao, L.-Q. Xia, S. Sun, K. Watanabe, T. Taniguchi, and P. Jarillo-Herrero, Robust supercon- ductivity in magic-angle multilayer graphene family, Nat. Mater. 21, 877 (2022)
work page 2022
- [26]
-
[27]
Z. Hao, A. M. Zimmerman, P. Ledwith, E. Khalaf, D. H. Najafabadi, K. Watanabe, T. Taniguchi, A. Vishwanath, and P. Kim, Electric field–tunable superconductivity in alternating-twist magic-angle trilayer graphene, Science 371, 1133 (2021)
work page 2021
-
[28]
X. Lu, P. Stepanov, W. Yang, M. Xie, M. A. Aamir, I. Das, C. Urgell, K. Watanabe, T. Taniguchi, G. Zhang, A. Bachtold, A. H. MacDonald, and D. K. Efetov, Su- perconductors, orbital magnets and correlated states in magic-angle bilayer graphene, Nature 574, 653 (2019)
work page 2019
-
[29]
M. Yankowitz, S. Chen, H. Polshyn, Y. Zhang, K. Watan- abe, T. Taniguchi, D. Graf, A. F. Young, and C. R. Dean, Tuning superconductivity in twisted bilayer graphene, Science 363, 1059 (2019)
work page 2019
-
[30]
M. Oh, K. P. Nuckolls, D. Wong, R. L. Lee, X. Liu, K. Watanabe, T. Taniguchi, and A. Yazdani, Evidence for unconventional superconductivity in twisted bilayer graphene, Nature 600, 240 (2021)
work page 2021
-
[31]
Y. Cao, V. Fatemi, A. Demir, S. Fang, S. L. Tomarken, J. Y. Luo, J. D. Sanchez-Yamagishi, K. Watanabe, T. Taniguchi, E. Kaxiras, R. C. Ashoori, and P. Jarillo- Herrero, Correlated insulator behaviour at half-filling in magic-angle graphene superlattices, Nature 556, 80 (2018)
work page 2018
-
[32]
P. Stepanov, I. Das, X. Lu, A. Fahimniya, K. Watanabe, T. Taniguchi, F. H. L. Koppens, J. Lischner, L. Levitov, and D. K. Efetov, Untying the insulating and supercon- ducting orders in magic-angle graphene, Nature 583, 375 (2020), 32632215
work page 2020
-
[33]
A. L. Sharpe, E. J. Fox, A. W. Barnard, J. Finney, K. Watanabe, T. Taniguchi, M. A. Kastner, and D. Goldhaber-Gordon, Emergent ferromagnetism near three-quarters filling in twisted bilayer graphene, Science 365, 605 (2019)
work page 2019
- [34]
-
[35]
P. Stepanov, M. Xie, T. Taniguchi, K. Watanabe, X. Lu, A. H. MacDonald, B. A. Bernevig, and D. K. Efetov, Competing Zero-Field Chern Insulators in Superconduct- ing Twisted Bilayer Graphene, Phys. Rev. Lett. 127, 197701 (2021)
work page 2021
-
[36]
I. Das, X. Lu, J. Herzog-Arbeitman, Z.-D. Song, K. Watanabe, T. Taniguchi, B. A. Bernevig, and D. K. Efetov, Symmetry-broken Chern insulators and Rashba-like Landau-level crossings in magic-angle bilayer graphene, Nat. Phys. 17, 710 (2021)
work page 2021
-
[37]
D. Rodan-Legrain, Y. Cao, J. M. Park, S. C. de la Bar- rera, M. T. Randeria, K. Watanabe, T. Taniguchi, and 10 P. Jarillo-Herrero, Highly tunable junctions and non-local Josephson effect in magic-angle graphene tunnelling de- vices, Nat. Nanotechnol. 16, 769 (2021)
work page 2021
-
[38]
F. K. de Vries, E. Portol´ es, G. Zheng, T. Taniguchi, K. Watanabe, T. Ihn, K. Ensslin, and P. Rickhaus, Gate- defined Josephson junctions in magic-angle twisted bi- layer graphene, Nat. Nanotechnol. 16, 760 (2021)
work page 2021
-
[39]
E. Portol´ es, S. Iwakiri, G. Zheng, P. Rickhaus, T. Taniguchi, K. Watanabe, T. Ihn, K. Ensslin, and F. K. de Vries, A tunable monolithic SQUID in twisted bilayer graphene, Nat. Nanotechnol. 17, 1159 (2022)
work page 2022
-
[40]
M. Perego, C. G. Agero, A. M. Tor` a, E. Portol´ es, A. O. Denisov, T. Taniguchi, K. Watanabe, F. Gaggioli, V. Geshkenbein, G. Blatter, T. Ihn, and K. Ensslin, Ex- perimental detection of vortices in magic-angle graphene, arXiv 10.48550/arXiv.2410.03508 (2024), 2410.03508
-
[41]
E. Portol´ es, M. Perego, P. A. Volkov, M. Toschini, Y. Kemna, A. Mestre-Tor` a, G. Zheng, A. O. Denisov, F. K. d. Vries, P. Rickhaus, T. Taniguchi, K. Watan- abe, J. H. Pixley, T. Ihn, and K. Ensslin, Quasiparticle and superfluid dynamics in Magic-Angle Graphene, Nat. Commun. 16, 4273 (2025)
work page 2025
-
[42]
M. Davydova, S. Prembabu, and L. Fu, Universal Joseph- son diode effect, Sci. Adv. 8, eabo0309 (2022)
work page 2022
- [43]
- [44]
-
[45]
Y.-M. Xie, D. K. Efetov, and K. T. Law, φ 0-Josephson junction in twisted bilayer graphene induced by a valley- polarized state, Phys. Rev. Res. 5, 023029 (2023)
work page 2023
-
[46]
M. Alvarado, P. Burset, and A. L. Yeyati, Intrinsic nonmagnetic ϕ 0 Josephson junctions in twisted bilayer graphene, Phys. Rev. Res. 5, L032033 (2023)
work page 2023
-
[47]
A. J. Annunziata, D. F. Santavicca, L. Frunzio, G. Cate- lani, M. J. Rooks, A. Frydman, and D. E. Prober, Tunable superconducting nanoinductors, Nanotechnol- ogy 21, 445202 (2010)
work page 2010
-
[48]
A. Barone and G. Patern` o, Physics and Applications of the Josephson Effect (John Wiley & Sons, Ltd, 1982) Chap. 5
work page 1982
-
[49]
D. L´ opez-N´ u˜ nez, A. Torras-Coloma, Q. P. Montserrat, E. Bertoldo, L. Cozzolino, G. Rius, M. Mart ´ ınez, and P. Forn-D ´ ıaz, Magnetic penetration depth of Aluminum thin films, arXiv 10.48550/arXiv.2311.14119 (2023), 2311.14119
-
[50]
L. Banszerus, C. W. Andersson, W. Marshall, T. Linde- mann, M. J. Manfra, C. M. Marcus, and S. Vaitiek˙ enas, Hybrid Josephson Rhombus: A Superconducting Ele- ment with Tailored Current-Phase Relation, Phys. Rev. X 15, 011021 (2025)
work page 2025
-
[51]
R. Jha, M. Endres, K. Watanabe, T. Taniguchi, M. Banerjee, C. Sch¨ onenberger, and P. Karnatak, Large Tunable Kinetic Inductance in a Twisted Graphene Su- perconductor, Phys. Rev. Lett. 134, 216001 (2025)
work page 2025
-
[52]
Tinkham, Introduction to Superconductivity , Vol
M. Tinkham, Introduction to Superconductivity , Vol. 2 (Dover Publications, 2004)
work page 2004
-
[53]
B. Sac´ ep´ e, M. Feigel’man, and T. M. Klapwijk, Quan- tum breakdown of superconductivity in low-dimensional materials, Nat. Phys. 16, 734 (2020)
work page 2020
-
[54]
J. A. Glick, M. A. Khasawneh, B. M. Niedzielski, R. Loloee, W. P. Pratt, N. O. Birge, E. C. Gingrich, P. G. Kotula, and N. Missert, Critical current oscilla- tions of elliptical Josephson junctions with single-domain ferromagnetic layers, J. Appl. Phys. 122, 133906 (2017)
work page 2017
-
[55]
Y. M. Ivanchenko and L. A. Zil’berman, The Joseph- son Effect in Small Tunnel Contacts, Sov. Phys. J. Exp. Theor. Phys. 28, 1272 (1969)
work page 1969
-
[56]
V. Ambegaokar and B. I. Halperin, Voltage Due to Ther- mal Noise in the dc Josephson Effect, Phys. Rev. Lett. 22, 1364 (1969)
work page 1969
-
[57]
W. F. Schiela, M. Mikalsen, D. Crawford, S. Ili´ c, W. M. Strickland, F. S. Bergeret, and J. Shabani, Gate-tunable polarity inversions and three-fold rotation symmetry of the superconducting diode effect, arXiv 10.48550/arXiv.2504.21470 (2025), 2504.21470
-
[58]
L. J. McGilly, A. Kerelsky, N. R. Finney, K. Shapovalov, E.-M. Shih, A. Ghiotto, Y. Zeng, S. L. Moore, W. Wu, Y. Bai, K. Watanabe, T. Taniguchi, M. Stengel, L. Zhou, J. Hone, X. Zhu, D. N. Basov, C. Dean, C. E. Dreyer, and A. N. Pasupathy, Visualization of moir´ e superlat- tices, Nat. Nanotechnol. 15, 580 (2020)
work page 2020
-
[59]
A. Sch¨ apers, J. Sonntag, L. Valerius, B. Pestka, J. Stras- das, K. Watanabe, T. Taniguchi, L. Wirtz, M. Morgen- stern, B. Beschoten, R. J. Dolleman, and C. Stampfer, Raman imaging of twist angle variations in twisted bi- layer graphene at intermediate angles, 2D Mater. 9, 045009 (2022)
work page 2022
-
[60]
A. Uri, S. Grover, Y. Cao, J. A. Crosse, K. Bagani, D. Rodan-Legrain, Y. Myasoedov, K. Watanabe, T. Taniguchi, P. Moon, M. Koshino, P. Jarillo-Herrero, and E. Zeldov, Mapping the twist-angle disorder and Landau levels in magic-angle graphene, Nature 581, 47 (2020)
work page 2020
-
[61]
Y. Choi, H. Kim, Y. Peng, A. Thomson, C. Lewandowski, R. Polski, Y. Zhang, H. S. Arora, K. Watanabe, T. Taniguchi, J. Alicea, and S. Nadj-Perge, Correlation- driven topological phases in magic-angle twisted bilayer graphene, Nature 589, 536 (2021)
work page 2021
-
[62]
R. J. Dolleman, A. Rothstein, A. Fischer, L. Klebl, L. Waldecker, K. Watanabe, T. Taniguchi, D. M. Kennes, F. Libisch, B. Beschoten, and C. Stampfer, Negative elec- tronic compressibility in charge islands in twisted bilayer graphene, Phys. Rev. B 109, 155430 (2024)
work page 2024
-
[63]
C. N. Lau, M. W. Bockrath, K. F. Mak, and F. Zhang, Reproducibility in the fabrication and physics of moir´ e materials, Nature 602, 41 (2022)
work page 2022
-
[64]
S. Reinhardt, T. Ascherl, A. Costa, J. Berger, S. Gronin, G. C. Gardner, T. Lindemann, M. J. Manfra, J. Fabian, D. Kochan, C. Strunk, and N. Paradiso, Link between supercurrent diode and anomalous Josephson effect re- vealed by gate-controlled interferometry, Nat. Commun. 15, 1 (2024)
work page 2024
-
[65]
M. D. Randle, M. Hosoda, R. S. Deacon, M. Ohtomo, P. Zellekens, K. Watanabe, T. Taniguchi, S. Okazaki, T. Sasagawa, K. Kawaguchi, S. Sato, and K. Ishibashi, Gate-Defined Josephson Weak-Links in Monolayer WTe2, Adv. Mater. 35, 2301683 (2023)
work page 2023
- [66]
- [67]
-
[68]
W. Albrecht, J. Moers, and B. Hermanns, HNF - Helmholtz Nano Facility, Journal of Large-Scale Research Facilities 3, 112 (2017)
work page 2017
-
[69]
J. M. Park, Y. Cao, K. Watanabe, T. Taniguchi, and P. Jarillo-Herrero, Flavour Hund’s coupling, Chern gaps and charge diffusivity in moir´ e graphene, Nature 592, 43 (2021)
work page 2021
-
[70]
K. Kim, M. Yankowitz, B. Fallahazad, S. Kang, H. C. P. Movva, S. Huang, S. Larentis, C. M. Corbet, T. Taniguchi, K. Watanabe, S. K. Banerjee, B. J. LeRoy, and E. Tutuc, van der Waals Heterostructures with High Accuracy Rotational Alignment, Nano Lett. 16, 1989 (2016)
work page 1989
-
[71]
T. Bisswanger, Z. Winter, A. Schmidt, F. Volmer, K. Watanabe, T. Taniguchi, C. Stampfer, and B. Beschoten, CVD Bilayer Graphene Spin Valves with 26 µ m Spin Diffusion Length at Room Temperature, Nano Lett. 2022, ,22 (2022)
work page 2022
-
[72]
L. Wang, I. Meric, P. Y. Huang, Q. Gao, Y. Gao, H. Tran, T. Taniguchi, K. Watanabe, L. M. Campos, D. A. Muller, J. Guo, P. Kim, J. Hone, K. L. Shepard, and C. R. Dean, One-Dimensional Electrical Contact to a Two- Dimensional Material, Science 342, 614 (2013)
work page 2013
-
[73]
T. Uwanno, T. Taniguchi, K. Watanabe, and K. Na- gashio, Electrically Inert h-BN/Bilayer Graphene Inter- face in All-Two-Dimensional Heterostructure Field Ef- fect Transistors, ACS Appl. Mater. Interfaces 10, 28780 (2018). Supporting Information - Gate-tunable Josephson diodes in magic-angle twiste d bilayer graphene A. Rothstein, 1, 2, ∗ R. J. Dolleman, ...
work page 2018
- [74]
- [75]
-
[76]
6 0 . 357055 0 . 0251004 0 . 480268 − 0. 043153 − 0. 625841 − 0. 228693 − 0. 459647 − 0. 946466 with “⊙ ” an element-wise multiplication of vectors, 1 − α = (1 − α 1, . . . , 1− α N )T , and sin( δ) = (sin( δ1), . . . , sin(δN ))T . For simulations, we employ the commonly used units Φ 0/ (2πI 0R) for time, I0 for current, I0R for voltage, and Φ 0 for flux ...
work page 2000
-
[77]
A. Pierret, D. Mele, H. Graef, J. Palomo, T. Taniguchi, K. Watan abe, Y. Li, B. Toury, C. Journet, P. Steyer, V. Gar- nier, A. Loiseau, J.-M. Berroir, E. Bocquillon, G. F` eve, C. Vois in, E. Baudin, M. Rosticher, and B. Pla¸ cais, Dielectric permittivity, conductivity and breakdown field of hexagonal b oron nitride, Mater. Res. Express 9, 065901 (2022)
work page 2022
-
[78]
A. Laturia, M. L. Van de Put, and W. G. Vandenberghe, Dielectri c properties of hexagonal boron nitride and transition metal dichalcogenides: from monolayer to bulk, npj 2D Mater. Ap pl. 2, 1 (2018)
work page 2018
-
[79]
Y. Cao, V. Fatemi, A. Demir, S. Fang, S. L. Tomarken, J. Y. Luo, J. D. Sanchez-Yamagishi, K. Watanabe, T. Taniguchi, E. Kaxiras, R. C. Ashoori, and P. Jarillo-Herrero, Correlated insula tor behaviour at half-filling in magic-angle graphene superlattices, Nature 556, 80 (2018)
work page 2018
-
[80]
Tinkham, Introduction to Superconductivity, Vol
M. Tinkham, Introduction to Superconductivity, Vol. 2 (Dover Publications, 2004)
work page 2004
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.