Above room temperature multiferroic tunnel junction with the altermagnetic metal CrSb
Pith reviewed 2026-05-23 00:02 UTC · model grok-4.3
The pith
The CrSb/In2Se3/Fe3GaTe2 heterostructure forms an above-room-temperature multiferroic tunnel junction with magnetically switchable TER and electrically tunable TMR.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The CrSb/In2Se3/Fe3GaTe2 heterostructure enables magnetically switchable TER, electrically tunable TMR, and dual-mode controllable spin filtering. Calculations with first-principles and nonequilibrium Green function methods show TMR up to 2308 percent, TER of 707 percent, and near-perfect spin filtering efficiency. Both TMR and TER remain considerable for either Cr or Sb interface termination. The transport performance is robust under bias voltage. These results establish an experimentally fabricable above-room-temperature multiferroic altermagnet-based magnetic tunnel junction.
What carries the argument
The CrSb/In2Se3/Fe3GaTe2 heterostructure, in which the altermagnetic CrSb supplies momentum-dependent spin splitting with zero net moment, the ferroelectric In2Se3 barrier supplies reversible polarization for TER, and the ferromagnetic Fe3GaTe2 electrode supplies conventional spin polarization for TMR.
If this is right
- Magnetically switchable tunneling electroresistance arises from ferroelectric polarization reversal.
- Electrically tunable tunneling magnetoresistance arises from the altermagnetic spin splitting interacting with the ferromagnetic electrode.
- Dual-mode controllable spin filtering reaches near-perfect efficiency in both parallel and antiparallel configurations.
- The same high TMR and TER values appear for both Cr-terminated and Sb-terminated interfaces.
- Transport metrics remain stable across a range of applied bias voltages.
Where Pith is reading between the lines
- The architecture points toward altermagnets serving as pinning layers in practical MTJs that avoid stray fields from net magnetization.
- Room-temperature operation with dual electric-magnetic control could simplify integration into existing semiconductor processes for sensing applications.
- Similar heterostructures using other altermagnets paired with different ferroelectrics could be tested to optimize the TER magnitude.
Load-bearing premise
The first-principles and nonequilibrium Green function calculations accurately capture the real interface electronic structure, polarization stability, and transport without defects, disorder, or temperature effects that would appear in fabricated devices.
What would settle it
Experimental fabrication of the CrSb/In2Se3/Fe3GaTe2 stack followed by direct measurement of TMR and TER under combined magnetic and electric field sweeps to test whether the observed ratios reach or fall short of the calculated 2308 percent TMR and 707 percent TER.
Figures
read the original abstract
Altermagnets with nonrelativistic momentum-dependent spin splitting and compensated net magnetic moments have recently garnered significant interest in spintronics, particularly as pinning layers in magnetic tunnel junctions (MTJs). However, room temperature (RT) altermagnet-based MTJs with tunable tunneling magnetoresistance (TMR) or electroresistance (TER) modulated by multiferroicity remain largely unexplored. Here, we propose an experimentally fabricable above-RT multiferroic MTJ, comprising an altermagnetic metal, ferroelectric barrier, and ferromagnetic metal-epitomized by a CrSb/In2Se3/Fe3GaTe2 heterostructure. Our calculations with first-principles and nonequilibrium Green function method indicate that the architecture enables magnetically switchable TER, electrically tunable TMR, and dual-mode controllable spin filtering. To disentangle the roles of ferroelectricity and the tunnel barrier, nonferroelectric Sb2Se3 and a vacuum gap are exploited as control cases. Remarkably, the system achieves TMR up to 2308%, TER of 707%, and near-perfect spin filtering efficiency. Both TMR and TER are considerable for CrSb/In2Se3/Fe3GaTe2 with either Cr or Sb interface. The transport performance is robust under bias voltage. These findings demonstrate the above-RT multiferroic altermagnet-based MTJs and highlight their exciting potential as a versatile platform for next-generation spin dynamics, magnetic sensing, and quantum logic nanodevices.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript proposes a CrSb/In2Se3/Fe3GaTe2 heterostructure as an above-room-temperature multiferroic magnetic tunnel junction that integrates an altermagnetic metal electrode, a ferroelectric barrier, and a ferromagnetic metal electrode. First-principles DFT combined with nonequilibrium Green's function (NEGF) transport calculations are reported to predict TMR ratios reaching 2308%, TER of 707%, near-100% spin filtering efficiency, magnetically switchable TER, electrically tunable TMR, and robustness under bias voltage, with control calculations using non-ferroelectric Sb2Se3 and vacuum barriers.
Significance. If the computational predictions are accurate for real interfaces, the work would demonstrate a versatile above-RT platform combining altermagnetism with multiferroic control, enabling dual-mode spin filtering and high-performance metrics not previously achieved in altermagnet-based MTJs. The use of control barriers to isolate ferroelectric effects is a positive methodological feature.
major comments (2)
- [Abstract] Abstract: The headline TMR (2308%) and TER (707%) values, together with the claim that the architecture 'enables' these in an 'experimentally fabricable' device, rest entirely on NEGF calculations performed on ideal, defect-free supercells at 0 K. No quantification is given of how atomic intermixing, vacancies, or finite-temperature fluctuations at the CrSb/In2Se3 and In2Se3/Fe3GaTe2 interfaces would alter the transmission probabilities or polarization stability; this assumption is load-bearing for the central performance and fabricability claims.
- [Abstract] Abstract and transport results: No error bars, convergence tests with respect to k-point sampling or supercell size, or direct validation against known experimental TMR/TER benchmarks for similar heterostructures are reported. The numerical precision of the quoted percentages therefore cannot be assessed, weakening the quantitative claims.
Simulated Author's Rebuttal
We thank the referee for the constructive comments on our manuscript. We address each major point below, clarifying the scope of our ideal-interface calculations while agreeing to strengthen the presentation of limitations where appropriate.
read point-by-point responses
-
Referee: [Abstract] Abstract: The headline TMR (2308%) and TER (707%) values, together with the claim that the architecture 'enables' these in an 'experimentally fabricable' device, rest entirely on NEGF calculations performed on ideal, defect-free supercells at 0 K. No quantification is given of how atomic intermixing, vacancies, or finite-temperature fluctuations at the CrSb/In2Se3 and In2Se3/Fe3GaTe2 interfaces would alter the transmission probabilities or polarization stability; this assumption is load-bearing for the central performance and fabricability claims.
Authors: Our DFT+NEGF results are obtained for ideal, defect-free supercells at zero temperature, which is the standard approach in first-principles transport studies to establish intrinsic upper-bound performance. The 'experimentally fabricable' statement rests on the known epitaxial compatibility of CrSb, In2Se3, and Fe3GaTe2 with existing growth techniques for similar van der Waals heterostructures. We agree that real interfaces may show reduced metrics due to imperfections and will add an explicit caveat in the abstract and discussion sections acknowledging this limitation of the ideal model. revision: yes
-
Referee: [Abstract] Abstract and transport results: No error bars, convergence tests with respect to k-point sampling or supercell size, or direct validation against known experimental TMR/TER benchmarks for similar heterostructures are reported. The numerical precision of the quoted percentages therefore cannot be assessed, weakening the quantitative claims.
Authors: Convergence with respect to k-point density and supercell size was verified during the calculations using standard dense meshes appropriate for the periodic structures. We will revise the methods section to report the specific k-point sampling and supercell dimensions employed. Direct experimental benchmarks for altermagnet-based multiferroic MTJs do not yet exist, as this architecture is new; the reported values are consistent with high TMR ratios obtained in related computational and experimental MTJ systems. We will also add a brief statement on numerical precision. revision: partial
- The quantification of how atomic intermixing, vacancies, or finite-temperature fluctuations at the interfaces would alter the transmission probabilities or polarization stability.
Circularity Check
No circularity: standard DFT+NEGF forward calculations
full rationale
The paper computes TMR, TER, and spin-filtering efficiencies via first-principles DFT combined with nonequilibrium Green's function transport on explicit atomic supercells of the CrSb/In2Se3/Fe3GaTe2 stack. These quantities are direct numerical outputs of the Schrödinger equation solution under the stated boundary conditions; they are not obtained by fitting parameters to the target observables, by self-definition, or by any self-citation chain that would render the result tautological. Control calculations with Sb2Se3 and vacuum barriers are likewise independent forward runs. No load-bearing uniqueness theorem, ansatz smuggling, or renaming of known results is present. The derivation chain is therefore self-contained against external benchmarks.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Standard first-principles DFT and NEGF methods accurately predict interface electronic structure and spin-dependent transport in the heterostructure.
Lean theorems connected to this paper
-
IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
Our calculations with first-principles and nonequilibrium Green function method indicate that the architecture enables magnetically switchable TER, electrically tunable TMR...
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
TMR up to 2308%, TER of 707%, and near-perfect spin filtering efficiency
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
L. Šmejkal, J. Sinova, and T. Jungwirth, Beyond Conventional Ferromagnetism and Antiferromagnetism: A Phase with Nonrelativistic Spin and Crystal Rotation Symmetry, Phys. Rev. X 12, 031042 (2022)
work page 2022
- [2]
- [3]
- [4]
-
[5]
L. Cao, Y . S. Ang, Q. Wu, and L. K. Ang, Electronic properties and spintronic applications of carbon phosphide nanoribbons, Phys. Rev. B 101, 035422 (2020)
work page 2020
-
[6]
C. Jin, J. Shang, X. Tang, X. Tan, S. C. Smith, C. Niu, Y . Dai, and L. Kou, Enhanced stability and stacking dependent magnetic/electronic properties of 2D monolayer FeTiO 3 on a Ti 2CO2 substrate, J. Mater. Chem. C 7, 15308 (2019)
work page 2019
- [7]
-
[8]
L. Šmejkal, J. Sinova, and T. Jungwirth, Emerging Research Landscape of Altermagnetism, Phys. Rev. X 12, 040501 (2022)
work page 2022
-
[9]
W. Sun, W. Wang, C. Yang, R. Hu, S. Yan, S. Huang, and Z. Cheng, Altermagnetism Induced by Sliding Ferroelectricity via Lattice Symmetry -Mediated Magnetoelectric Coupling, Nano Lett. 24, 11179 (2024). 24
work page 2024
-
[10]
Y . Wu, L. Deng, X. Yin, J. Tong, F. Tian, and X. Zhang, Valley -Related Multipiezo Effect and Noncollinear Spin Current in an Altermagnet Fe2Se2O Monolayer, Nano Lett. 24, 10534 (2024)
work page 2024
-
[11]
Y . Zhu, T. Chen, Y . Li, L. Qiao, X. Ma, C. Liu, T. Hu, H. Gao, and W. Ren, Multipiezo Effect in Altermagnetic V2SeTeO Monolayer, Nano Lett. 24, 472 (2024)
work page 2024
- [12]
-
[13]
S. Reimers, L. Odenbreit, L. Šmejkal, V . N. Strocov, P. Constantinou, A. B. Hellenes, R. Jaeschke Ubiergo, W. H. Campos, V . K. Bharadwaj, A. Chakraborty, T. Denneulin, W. Shi, R. E. Dunin-Borkowski, S. Das, M. Kläui, J. Sinova, and M. Jourdan, Direct observation of altermagnetic band splitting in CrSb thin films, Nat. Commun. 15, 2116 (2024)
work page 2024
-
[14]
Z. Zhou, X. Cheng, M. Hu, R. Chu, H. Bai, L. Han, J. Liu, F. Pan, and C. Song, Manipulation of the altermagnetic order in CrSb via crystal symmetry, Nature 638, 645 (2025)
work page 2025
- [15]
-
[16]
M. Chilcote, A. R. Mazza, Q. Lu, I. Gray, Q. Tian, Q. Deng, D. Moseley, A. H. Chen, J. Lapano, J. S. Gardner, G. Eres, T. Z. Ward, E. Feng, H. Cao, V . Lauter, M. A. McGuire, R. Hermann, D. Parker, M. G. Han, A. Kayani, G. Rimal, L. Wu, T. R. Charlton, R. G. Moore, and M. Brahlek, Stoichio metry‐ Induced Ferromagnetism in Altermagnetic Candidate MnTe, Adv...
work page 2024
-
[17]
S. A. Egorov and R. A. Evarestov, Colossal Spin Splitting in the Monolayer of the Collinear Antiferromagnet MnF2, J. Phys. Chem. Lett. 12, 2363 (2021)
work page 2021
-
[18]
L. Šmejkal, R. González -Hernández, T. Jungwirth, and J. Sinova, Crystal time -reversal symmetry breaking and spontaneous Hall effect in collinear antiferromagnets, Sci. Adv. 6, eaaz8809 (2020)
work page 2020
-
[19]
H.-Y . Ma, M. Hu, N. Li, J. Liu, W. Yao, J. -F. Jia, and J. Liu, Multifunctional antiferromagnetic materials with giant piezomagnetism and noncollinear spin current, Nat. Commun. 12, 2846 (2021)
work page 2021
-
[20]
D. Wang, H. Wang, L. Liu, J. Zhang, and H. Zhang, Electric -Field-Induced Switchable Two-Dimensional Altermagnets, Nano Lett. 25, 498 (2025)
work page 2025
-
[21]
A. Kaur and A. De Sarkar, Recent advances in theoretical investigations of sliding ferroelectricity in layered and van der Waals two-dimensional materials, J. Phys.: Conden. Matter 37, 253001 (2025)
work page 2025
-
[22]
S. N. Kajale, J. Hanna, K. Jang, and D. Sarkar, Two-dimensional magnetic materials for spintronic applications, Nano Res. 17, 743 (2024)
work page 2024
-
[23]
J. W. Lee, J. Han, B. Kang, Y . J. Hong, S. Lee, and I. Jeon, Strategic Development of Memristors for Neuromorphic Systems : Lo w‐Power and Reconfigurable Operation, Adv. Mater. 37, 2413916 (2025)
work page 2025
-
[24]
H. Yang, S. O. Valenzuela, M. Chshiev, S. Couet, B. Dieny, B. Dlubak, A. Fert, K. Garello, M. Jamet, D. -E. Jeong, K. Lee, T. Lee, M. -B. Martin, G. S. Kar, P . Sénéor, H. -J. Shin, and S. Roche, Two-dimensional materials prospects for non-volatile spintronic memories, Nature 606, 663 (2022)
work page 2022
-
[25]
B. Chen, M. Zeng, K. H. Khoo, D. Das, X. Fong, S. Fukami, S. Li, W. Zhao, S. S. P. Parkin, S. N. Piramanayagam, and S. T. Lim, Spintronic devices for high -density memory and neuromorphic computing – A review, Mater. Today 70, 193 (2023)
work page 2023
- [26]
-
[27]
Q. Cui, Y . Zhu, X. Yao, P. Cui, and H. Yang, Giant spin -Hall and tunneling magnetoresistance effects based on a two -dimensional nonrelativistic antiferromagnetic metal, Phys. Rev. B 108, 024410 (2023)
work page 2023
-
[28]
K. Samanta, D. -F. Shao, and E. Y . Tsymbal, Spin Filtering with Insulating Altermagnets, Nano Lett. 25, 3150 (2025)
work page 2025
-
[29]
F. Liu, Z. Zhang, X. Yuan, Y . Liu, S. Zhu, Z. Lu, and R. Xiong, Giant tunneling magnetoresistance in insulated altermagnet/ferromagnet junctions induced by spin -dependent tunneling effect, Phys. Rev. B 110, 134437 (2024)
work page 2024
-
[30]
B. Chi, L. Jiang, Y . Zhu, G. Yu, C. Wan, J. Zhang, and X. Han, Crystal-facet-oriented altermagnets for detecting ferromagnetic and antiferromagnetic states by giant tunneling magnetoresistance, Phys. Rev. Appl. 21, 034038 (2024)
work page 2024
-
[31]
P. Heller and G. B. Benedek, Nuclear Magnetic Resonance in MnF 2 Near the Critical Point, Phys. Rev. Lett. 8, 428 (1962)
work page 1962
-
[32]
X. Zhou, W. Feng, R. -W. Zhang, L. Šmejkal, J. Sinova, Y . Mokrousov, and Y . Yao, Crystal Thermal Transport in Altermagnetic RuO2, Phys. Rev. Lett. 132, 056701 (2024)
work page 2024
-
[33]
J. Liu, J. Zhan, T. Li, J. Liu, S. Cheng, Y . Shi, L. Deng, M. Zhang, C. Li, J. Ding, Q. Jiang, M. Ye, Z. Liu, Z. Jiang, S. Wang, Q. Li, Y . Xie, Y . Wang, S. Qiao, J. Wen, Y . Sun, and D. Shen, Absence of Altermagnetic Spin Splitting Character in Rutile Oxide RuO2, Phys. Rev. Lett. 133, 176401 (2024)
work page 2024
-
[34]
X. Duan, J. Zhang, Z. Zhu, Y . Liu, Z. Zhang, I. Žutić, and T. Zhou, Antiferroelectric Altermagnets: Antiferroelectricity Alters Magnets, Phys. Rev. Lett. 134, 106801 (2025)
work page 2025
-
[35]
M. Gu, Y . Liu, H. Zhu, K. Yananose, X. Chen, Y . Hu, A. Stroppa, and Q. Liu, Ferroelectric Switchable Altermagnetism, Phys. Rev. Lett. 134, 106802 (2025)
work page 2025
-
[36]
Z. Yan, D. Qiao, W. Lu, X. Dong, and X. Xu, Magnetic order dependent giant tunneling magnetoresistance and electroresistance in van der Waals antiferromagnetic -multiferroic tunnel junctions, Phys. Rev. B 111, 045404 (2025)
work page 2025
-
[37]
Y . Feng, J. Han, K. Zhang, X. Lin, G. Gao, Q. Yang, and S. Meng, van der Waals multiferroic tunnel junctions based on sliding multiferroic layered VSi2N4, Phys. Rev. B 109, 085433 (2024)
work page 2024
-
[38]
J. Ding, Z. Jiang, X. Chen, Z. Tao, Z. Liu, T. Li, J. Liu, J. Sun, J. Cheng, J. Liu, Y . Yang, R. Zhang, L. Deng, W. Jing, Y . Huang, Y . Shi, M. Ye, S. Qiao, Y . Wang, Y . Guo, D. Feng, and D. Shen, Large Band Splitting in g-Wave Altermagnet CrSb, Phys. Rev. Lett. 133, 206401 (2024)
work page 2024
-
[39]
L. Han, X. Fu, R. Peng, X. Cheng, J. Dai, L. Liu, Y . Li, Y . Zhang, W. Zhu, H. Bai, Y . Zhou, S. Liang, C. Chen, Q. Wang, X. Chen, L. Yang, Y . Zhang, C. Song, J. Liu, and F. Pan, Electrical 180° switching of Néel vector in spin-splitting antiferromagnet, Sci. Adv. 10, eadn0479 (2024)
work page 2024
- [40]
-
[41]
W. Han, Z. Wang, S. Guan, J. Wei, Y . Jiang, L. Zeng, L. Shen, D. Yang, and H. Wang, Recent advances of phase transition and ferroelectric device in two -dimensional In2Se3, Appl. Phys. Rev. 11, 021314 (2024)
work page 2024
-
[42]
C. Cui, W.-J. Hu, X. Yan, C. Addiego, W. Gao, Y . Wang, Z. Wang, L. Li, Y . Cheng, P. Li, X. Zhang, H. N. Alshareef, T. Wu, W. Zhu, X. Pan, and L. -J. Li, Intercorrelated In -Plane and Out -of-Plane Ferroelectricity in Ultrathin Two -Dimensional Layered Semiconductor In 2Se3, Nano Lett. 18, 1253 (2018). 26
work page 2018
- [43]
-
[44]
J. P. Perdew, K. Burke, and M. Ernzerhof, Generalized Gradient Approximation Made Simple, Phys. Rev. Lett. 77, 3865 (1996)
work page 1996
-
[45]
S. M. Farzaneh and S. Rakheja, Intrinsic spin Hall effect in topological insulators: A first-principles study, Phys. Rev. Mater. 4, 114202 (2020)
work page 2020
-
[46]
H. Zhang, C.-X. Liu, X.-L. Qi, X. Dai, Z. Fang, and S.-C. Zhang, Topological insulators in Bi2Se3, Bi2Te3 and Sb2Te3 with a single Dirac cone on the surface, Nat. Phys. 5, 438 (2009)
work page 2009
-
[47]
W. Liu, X. Peng, C. Tang, L. Sun, K. Zhang, and J. Zhong, Anisotropic interactions and strain-induced topological phase transition in Sb2Se3 and Bi2Se3, Phys. Rev. B 84, 245105 (2011)
work page 2011
-
[48]
G. Kresse and J. Furthmüller, Efficient iterative schemes for ab initio total -energy calculations using a plane-wave basis set, Phys. Rev. B 54, 11169 (1996)
work page 1996
- [49]
-
[50]
G. Yang, Z. Li, S. Yang, J. Li, H. Zheng, W. Zhu, Z. Pan, Y . Xu, S. Cao, W. Zhao, A. Jana, J. Zhang, M. Ye, Y . Song, L.-H. Hu, L. Yang, J. Fujii, I. V obornik, M. Shi, H. Yuan, Y . Zhang, Y . Xu, and Y . Liu, Three-dimensional mapping of the altermagnetic spin splitting in CrSb, Nat. Commun. 16, 1442 (2025)
work page 2025
-
[51]
See Supplemental Material for band structures of Fe 3GaTe2 under different U values; high-symmetry points within Brillouin zone; the spin -, atomic - and orbital-resolved band structures; LDOS and PDDOS; transmission pathways; MTJs; and transmission coefficients
-
[52]
Y . Xi, H. Shi, J. Zhang, H. Li, N. Cheng, H. Xu, J. Liu, K. Li, H. Guo, H. Feng, J. Wang, W. Hao, and Y . Du, Large Magnetic Anisotropy in van der Waals Ferromagnet Fe 3GaTe2 above Room Temperature, J. Phys. Chem. Lett. 15, 10802 (2024)
work page 2024
- [53]
- [54]
- [55]
- [56]
- [57]
- [58]
-
[59]
X. Li, J. -T. Lü, J. Zhang, L. You, Y . Su, and E. Y . Tsymbal, Spin-Dependent Transport in van der Waals Magnetic Tunnel Junctions with Fe3GeTe2 Electrodes, Nano Lett. 19, 5133 (2019). 27
work page 2019
- [60]
-
[61]
X. Li, M. Zhu, Y . Wang, F. Zheng, J. Dong, Y . Zhou, L. You, and J. Zhang, Tremendous tunneling magnetoresistance effects based on van der Waals room-temperature ferromagnet Fe3GaTe2 with highly spin-polarized Fermi surfaces, Appl. Phys. Lett. 122, 082404 (2023)
work page 2023
- [62]
-
[63]
S. Xie, M. Shiffa, M. Shiffa, Z. R. Kudrynskyi, O. Makarovskiy, Z. D. Kovalyuk, W. Zhu, K. Wang, and A. Patanè, Van der Waals interfaces in multilayer junctions for ultraviolet photodetection, npj 2D Mater. Appl. 6, 61 (2022)
work page 2022
-
[64]
H. -x. Liu, Y . Honda, T. Taira, K. -i. Matsuda, M. Arita, T. Uemura, and M. Yamamoto, Giant tunneling magnetoresistance in epitaxial Co 2MnSi/MgO/Co2MnSi magnetic tunnel junctions by half-metallicity of Co2MnSi and coherent tunneling, Appl. Phys. Lett. 101, 132418 (2012)
work page 2012
-
[65]
T. Ma, Y . Zhu, P. A. Dainone, T. Chen, X. Devaux, C. Wan, S. Migot, G. Lengaigne, M. Vergnat, Y . Yan, X. Han, and Y . Lu, Large Sign Reversal of Tunneling Magnetoresistance in an Epitaxial Fe/MgAlOx/Fe4N Magnetic Tunnel Junction, ACS Appl. Electron. Mater. 5, 5954 (2023)
work page 2023
-
[66]
Y . Su, X. Li, M. Zhu, J. Zhang, L. You, and E. Y . Tsymbal, Van der Waals Multiferroic Tunnel Junctions, Nano Lett. 21, 175 (2021)
work page 2021
-
[67]
H. Bai, X. Li, H. Pan, P. He, Z.-a. Xu, and Y . Lu, Van der Waals Antiferroelectric Magnetic Tunnel Junction: A First -Principles Study of a CrSe 2/CuInP2S6/CrSe2 Junction, ACS Appl. Mater. Inter. 13, 60200 (2021)
work page 2021
- [68]
-
[69]
J. P. Velev, C.-G. Duan, J. D. Burton, A. Smogunov, M. K. Niranjan, E. Tosatti, S. S. Jaswal, and E. Y . Tsymbal, Magnetic Tunnel Junctions with Ferroelectric Barriers: Prediction of Four Resistance States from First Principles, Nano Lett. 9, 427 (2009)
work page 2009
-
[70]
Z. Cui, B. Sa, K. -H. Xue, Y . Zhang, R. Xiong, C. Wen, X. Miao, and Z. Sun, Magnetic-ferroelectric synergic control of multilevel conducting states in van der Waals multiferroic tunnel junctions towards in-memory computing, Nanoscale 16, 1331 (2024)
work page 2024
-
[71]
X.-H. Guo, L. Zhu, Z. -L. Cao, and K. -L. Yao, Tunable multiple nonvolatile resistance states in a MnSe-based van der Waals multiferroic tunnel junction, Phys. Chem. Chem. Phys. 26, 3531 (2024). 28 Figures and Tables FIG. 1. Top (a-e) and side (f-j) views for the crystal structures of CrSb bulk, Fe3GaTe2 bulk, In2Se3 monolayers with opposite ferroelectric...
work page 2024
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.