The first Online SPICE-Workshop on 2D van der Waals Spin Systems has been successfully completed. Scientists from all over the world have attended our workshop from 4th to 7th August, 2020. Thank you for your active participation!
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07.08.2020 – The first Online SPICE-Workshop
On-line SPICE-SPIN+X Seminars
On-line Seminar: 19.08.2020 - 15:00 (CET)
Antiferromagnetic Insulatronics: Spintronics without magnetic fields
Mathias Kläui, JGU Mainz
While known for a long time, antiferromagnetically ordered systems have previously been considered, as expressed by Louis Néel in his Nobel Prize Lecture, to be “interesting but useless”. However, since antiferromagnets potentially promises faster operation, enhanced stability with respect to interfering magnetic fields and higher integration due to the absence of dipolar coupling, they could potentially become a game changer for new spintronic devices. The zero net moment makes manipulation using conventional magnetic fields challenging. However recently, these materials have received renewed attention due to possible manipulation based on new approaches such as photons [1] or spin-orbit torques [2].
In this talk, we will present an overview of the key features of antiferromagnets to potentially functionalize their unique properties. This includes writing, reading and transporting information using antiferromagnets.
We recently realized switching in the metallic antiferromagnet Mn2Au by intrinsic staggered spin-orbit torques [3,4] and characterize the switching properties by direct imaging. While switching by staggered intrinsic spin-orbit torques in metallic AFMs requires special structural asymmetry, interfacial non-staggered spin-orbit torques can switch multilayers of many insulating AFMs capped with heavy metal layers.
We probe switching and spin transport in selected collinear insulating antiferromagnets, such as NiO [5-7], CoO [8,9] and hematite [10,11]. In NiO and CoO we find that there are multiple switching mechanisms that result in the reorientation of the Néel vector and additionally effects related to electromigration of the heavy metal layer can obscure the magnetic switching [5,7,9]. For the spin transport, spin currents are generated by heating as resulting from the spin Seebeck effect and by spin pumping measurements and we find in vertical transport short (few nm) spin diffusion lengths [6,8].
For hematite, however, we find in a non-local geometry that spin transport of tens of micrometers is possible [10,11]. We detect a first harmonic signal, related to the spin conductance, that exhibits a maximum at the spin-flop reorientation, while the second harmonic signal, related to the Spin Seebeck conductance, is linear in the amplitude of the applied magnetic field [10]. The first signal is dependent on the direction of the Néel vector and the second one depends on the induced magnetic moment due to the field. We identify the domain structure as the limiting factor for the spin transport [11]. We recently also achieved transport in the easy plane phase [12], which allows us to obtain long distance spin transport in hematite even at room temperature [12]. From the power and distance dependence, we unambiguously distinguish long-distance transport based on diffusion [10,11] from predicted spin superfluidity that can potentially be used for logic [13].
A number of excellent reviews are available for further information on recent developments in the field [14].
PDF file of the talk available here
References
[1] A. Kimel et al., Nature 429, 850 (2004). [2] J. Zelezny et al., Phys. Rev. Lett. 113, 157201 (2014); P. Wadley et al., Science 351, 587 (2016). [3] S. Bodnar et al., Nature Commun. 9, 348 (2018) [4] S. Bodnar et al., Phys. Rev. B 99, 140409(R) (2019). [5] L. Baldrati et al., Phys. Rev. Lett. 123, 177201 (2019) [6] L. Baldrati et al., Phys. Rev. B 98, 024422 (2018); L. Baldrati et al. Phys. Rev. B 98, 014409 (2018) [7] F. Schreiber et al., arxiv:2004.13374 (in press 2020) [8] J. Cramer et al., Nature Commun. 9, 1089 (2018) [9] L. Baldrati et al., Phys. Rev. Lett. 125, 077201 (2020) [10] R. Lebrun et al., Nature 561, 222 (2018). [11] A. Ross et al., Nano Lett. 20, 306 (2020). [12] R. Lebrun et al., arxiv:2005.14414 (2020). [13] Y. Tserkovnyak et al., Phys. Rev. Lett. 119, 187705 (2017). [14] Rev. Mod. Phys. 90, 15005 (2018); Nat. Phys. 14, 200-242 (2018); Adv. Mater. 32, 1905603 (2020)On-line SPICE-SPIN+X Seminars
On-line Seminar: 26.08.2020 - 15:00 (CET)
Magnetic Matchmaking: Hybrid Magnon Modes
Axel Hoffmann, University of Illinois
Hybrid dynamic excitations have gained increased interest due to their potential impact on coherent information processing. Towards this end, magnons, the fundamental excitation quant of magnetically ordered systems, are of particular interest, since they can be easily tuned by external magnetic fields and interact with a wide range of other excitations, such as microwave and optical photons, phonons, and other magnons.1 We have explored recently the integration of permalloy (Ni80Fe20) thin film structures into hybrid magnon systems. By combining permalloy structures with high-quality superconducting microwave resonators, we demonstrated strong magnon-photon coupling in co-planar, on-chip geometry, which is readily scalable to more complex devices.2 Furthermore, we demonstrated strong coupling of permalloy magnons to standing magnon modes in yttrium iron garnet films, which revealed the importance of dampin-like torques originating from spin pumping.3 Lastly, we demonstrated how the coupling between magnons in Ni and surface acoustic waves in LiNbO3 can be used to modulate phonon propagation.4
This work was supported by the U.S. Department of Energy, Office of Science, Materials Sciences and Engineering Division.
PDF file of the talk available here
References:
1. Y. Li, et al., arXiv:2006.16158.
2. Y. Li, et al., Phys. Rev. Lett. 123, 107701 (2019).
3. Y. Li, et al., Phys. Rev. Lett. 124, 117202 (2020).
4. C. Zhao, et al., Phys. Rev. Appl. 13, 054032 (2020).
New Opportunities for Charge and Spin in the 2D Magnet RuCl3
Kenneth Burch
Precise control of electronic charge at the nanoscale has been crucial in creating new phases of matter and devices. Here I will present results on the 2D magnet RuCl3 that demonstrate it is able to induce large charge on short length scales in other materials. I will discuss its ability to work with various systems, and potential for control via relative twist angle. I will also review the limitations of this technique in terms of ultimate charge doping and homogeneity. Time permitting I will briefly discuss the unique magnetic excitations in this system useful for topological computing, and implications for heterostructures of RuCl3 with other 2D magnets.
Magnon transport in 2D (anti-)ferromagnets
Bart van Wees
In recent years it was demonstrated that magnons can be efficient transporters of spins, making new devices and functionalities possible with (insulating) magnonic systems. I will give an introduction into magnon spin transport in ferro/ferri/and anti-ferrro magnetic systems. I will discuss how charge current information can be transformed into (electronic) spin information by the spin Hall effect, which can then generate a magnon spin current in the ferrimagnetic insulators yttrium iron garnet (YIG) [1]. Magnon spins can then be detected via the inverse spin Hall effect, and converted back into a charge signal. These experiments have led to a better understanding of electrically and thermally induced magnon currents (spin Seebeck effect) and emphasize the role of the nonequilibrium magnon chemical potential as the driving force for magnon currents [2] Based on these concepts a magnon transistor geometry was fabricated in which the magnon density was controlled by a magnon injecting gate electrode [3]. It was also shown that magnons in antiferromagnets can effectively transport spins, and experiments demonstrated this in multilayer 2D Van der Waals antiferromagnets[4] I will discuss our recent results on magnon spin caloritronics, including magnon spin Seebeck effect and anomalous Nernst effects, in CrBr3 based ferromagnetic van der Waals systems.
- J. Cornelissen et al., Nat. Phys. 11, 1022 (2015)
- J. Cornelissen et al., Phys. Rev. B94, 014412 (2016)
- J. Cornelissen et al., Phys. Rev. Lett. 120, 097702 (2018)
- Xing et al., Phys. Rev. X9, 011026 (2019)
- Liu et al., Phys. Rev. B 101, 205407 (2020)
Poster Session
Poster 24 | Kingshuk Sarkar | Tel Aviv University | Datta-Das Spin FET under various magnetic fields |
Poster 25 | Hadar Steinberg | Hebrew University of Jerusalem | Spectroscopy of Layered SCs with vdW Tunnel Jcns |
Poster 26 | Bálint Szentpéteri | Budapest University of Technology and Economics | Measurement of spin-orbit interaction strength |
Poster 27 | Alfredo Tlahuice | UANL | TBA |
Poster 28 | Jesus Carlos Toscano Figueroa | University of Manchester | Spin injection enhancement and spin-anisotropy in functionalized graphene |
Poster 29 | Toyo Kazu Yamada | Chiba University, Japan | Molecular Hopping in a 2D Carbon Monoxide Film |
Poster 30 | Hongxin Yang | Chinese Academy of Sciences | DMI of 2D Janus Structure |
Poster 31 | Meghdad Yazdani Hamid | Ayatollah Boroujerdi University | Effect of the strain on the transverse conductivity of Sr2RuO4 |
Poster 32 | Yevhen Zabila | Institute of Nuclear Physics PAS | Bismuth-based flexible magnetic sensors |
Poster 33 | Bing Zhao | Chalmers University of Technology | Conventional and unconventional CSC in WTe2 |
Poster Session
Poster 13 | Mátyás Kocsis | Department of Physics, BUTE | Tuning the nonreciprocal resistance of BiTeBr |
Poster 14 | Kinga Lasek | University of South Florida | Molecular Beam Epitaxy of Self-Intercalated Transition Metal Tellurides |
Poster 15 | Soo Yeon Lim | Sogang University | Thickness dependent magnetic transition of MnPS3 |
Poster 16 | Mingzu Liu | The Pennsylvania State University | Tunable RT FM in 1L V-WS2 & V-WSe2 via CVD |
Poster 17 | Francisco Munoz | Universidad de Chile | Magnon Hall Effect in CrI3-based vdW systems |
Poster 18 | Tianxiao Nie | Beihang University | 2D ferromagnetic materials above room temperature |
Poster 19 | Sergey Nikolaev | Tokyo Institute of Technology | Realistic modelling of monolayer NbS2 and NbSe2 |
Poster 20 | Armando Pezo | Federal University of ABC | TMDC/Graphene an ab initio study |
Poster 21 | Charis Quay | UniversitÈ Paris-Saclay | Tunneling spectroscopy of few-monolayer NbSe2 |
Poster 22 | Akhil Rajan | University of St Andrews | Morphology control of monolayer transition metal dichalcogenides by MBE |
Poster 23 | Patrick Reiser | University of Basel | Scanning NV Magnetometry of 2D Magnetism |
Poster Session
Poster 1 | Himanshu Bangar | Indian Institute of Technology Delhi | Spin pumping from Ni80Fe20 into monolayer TMD |
Poster 2 | Fernando Bartolome | ICMA, Universidad de Zaragoza - CSIC | Magnetism of FePc/Ag(110) + O2 Monolayer Phases |
Poster 3 | Magdalena Birowska | University of Warsaw, Faculty of Physics, Poland | 2D magnetic crystal: An ab initio study of MnPS3 |
Poster 4 | Adam Budniak | Technion - Israel Institute of Technology | Exfoliated CrPS4 with promising photoconductivity |
Poster 5 | Xin Chen | Department of Physics and Astronomy, Uppsala University | 3d Transition Metal Clusters on Defected Graphene |
Poster 6 | Victor Manuel Garcia-Suarez | University of Oviedo | Electronics without bridging components |
Poster 7 | Md Anamul Hoque | Chalmers University of Technology | Charge - spin conversion in layered semimetal |
Poster 8 | Bogdan Karpiak | Chalmers University of Technology | Magnetic proximity in graphene/CGT heterostructure |
Poster 9 | Daljit Kaur | DAV University, Jalandhar | Magnetic investigations in VSe2 and CrSe2 nanorods |
Poster 10 | Roland Kawakami | The Ohio State University | Epitaxial growth of van der Waals magnets |
Poster 11 | Liqin Ke | Ames Laboratory, U.S. Department of Energy | Electron correlations and spin excitations in CrI3 |
Poster 12 | Safe Khan | UCL | Intercalating sodium atoms in a vdWs magnet |
2D Magnets, Heterostructures, and Spintronic Devices
Cheng Gong
Magnetism, one of the most fundamental physical properties, has revolutionized significant technologies such as data storage and biomedical imaging, and continues to bring forth new phenomena in emerging materials and reduced dimensions. The recently discovered magnetic 2D van der Waals materials (hereafter abbreviated as “2D magnets”) provide ideal platforms to enable the atomic-thin, flexible, lightweight magneto-optic and magnetoelectric devices. The seamless integration of 2D magnets with dissimilar electronic and photonic materials further opens up exciting possibilities for unprecedented properties and functionalities. In this tutorial, I will start with the fundamentals on 2D magnetism, and continue to speak on our experimental observation of 2D ferromagnet, analyze the current progress and the existing challenges in this emerging field, and show how we push the boundary by exploring the potential of 2D antiferromagnets for spintronics.
Quantum Phase Transition and Ising Superconductivity in transition metal dichalcogenides
Jianting Ye
Many recent discoveries on novel electronic states were made on 2D materials. Especially, by making artificial bilayer systems, new electronic states such as superconductivity and ferromagnetism have been reported. This talk will discuss quantum phase transitions and Ising superconductivity induced in 2D transition metal dichalcogenides. Using ionic gating, quantum phases such as superconductivity can be induced by field-effect on many 2D materials. In transition metal dichalcogenides, Ising-like paring states can form at K and K’ point of the hexagonal Brillouin zone. Also, we will discuss how to couple two Ising superconducting states through Josephson coupling by inducing superconductivity symmetrically in a suspended bilayer. This method can access electronic states with broken local inversion symmetry while maintaining the global inversion symmetry [3]. Controlling the Josephson coupling and spin-orbit coupling is an essential step for realizing many exotic electronics states predicted for the coupled bilayer superconducting system with strong spin-orbit interactions.
[1] Lu, J. M. Zheliuk O, et al., Science 350 1353 (2015).[2] Lu, J. M. Zheliuk O, et al., Proceedings of the National Academy of Sciences 115 3551 (2018).
[3] Zheliuk O, Lu, J. M., et al., Nature Nanotechnology 14 1123 (2019).