News and posts

Thin layers of CrBr3 and CrI3: reconaissance ventures into 2D magnetism

Maciej Koperski

The magnetism of chromium has been investigated for almost a century now, providing substantial knowledge about its electronic configuration. Extensive research has been conducted regarding the physics of valence electrons from d-shell, which is fundamentally important for understanding the mechanisms of magnetic ordering. Interestingly, chromium atom, exhibiting a stable electronic configuration exempting from Hund’s rules, has half-filled 3d shell, which leads to manifestation of robust magnetic effects in a variety of structures. Recently, attention has been refocused on chromium trihalides (CrCl3, CrBr3 and CrI3), which constitute a group of electrically insulating layered materials displaying magnetic ordering at low temperatures, as established by inspection of bulk crystals carried out few decades ago. The progress of mechanical exfoliation techniques, performed in a controlled argon atmosphere, enables now isolation of thin layers (down to monolayers) and their incorporation in van der Waals heterostructures.
Initial reports demonstrated layer-dependent ferromagnetic and anti-ferromagnetic order below Curie temperature using Kerr rotation measurements as magnetization probe. These appealing findings motivate further study to uncover the underlying microscopic mechanisms. One possible path to learn about the electronic structure and characteristics of electronic states via optical methods involves investigations of emission and absorption processes. Here, we present detailed optical studies of exfoliated films of CrBr3 and CrI3 to demonstrate that the emergent interband luminescence has molecular-like character (most likely due to formation of Frenkel-type excitons) and the details of the structure of emission resonances can be explained by Franck-Condon principle involving multiple phonon modes. The photoluminescence studies unveil unambiguous signatures of coupling between the magnetic moments of Cr3+ ions with band carriers, offering insight into fundamental properties of these novel magnetic structures and opening up new routes for potential applications of 2D systems.

Emergent properties of 2D magnets and their heterostructures explored by MBE

Masaki Nakano

 

Bottom-up molecular-beam epitaxy (MBE) provides a complementary approach to top-down mechanical exfoliation in 2D materials research. A great success lies in the application of MBE-grown large-area monolayer films to ARPES and STM/STS studies, unveiling emergent monolayer properties of various 2D materials. Considering the research history of semiconductors and oxides, however, one of the biggest advantages of MBE-based approach should be to create novel material systems unachievable by bulk-based approach and examine their transport phenomena, although such examples are very much limited presumably due to difficulties in making high-enough quality samples.

 

We have recently developed a fundamental route to layer-by-layer epitaxial growth of a wide variety of 2D materials and their heterostructures on insulating substrates by MBE [1-7], opening a door for exploration of emergent transport phenomena of 2D materials arising at the monolayer limit and at the interface between dissimilar materials even based on hardly-cleavable, chemically-unstable, and/or thermodynamically-metastable compounds. In this presentation, I will introduce our recent achievements in particular on the MBE-grown 2D magnets and their heterostructures, including observation of the emergent itinerant 2D ferromagnetism with intrinsic spin polarization in hardly-cleavable compound that are missing in its bulk counterpart [4], as well as control of its magnetic properties by the magnetic proximity effect across the van der Waals interface [7].

 

Reference:

[1] M. Nakano et al., Nano Lett. 17, 5595 (2017).

[2] Y. Wang et al., Appl. Phys. Lett. 113, 073101 (2018).

[3] Y. Kashiwabara et al., Adv. Funct. Mater. 29, 1900354 (2019).

[4] M. Nakano et al., Nano Lett. 19, 8806 (2019).

[5] Y. Tanaka et al., Nano Lett. 20, 1725 (2020).

[6] H. Matsuoka et al., Rhys. Rev. Research 2, 012064(R) (2020).

[7] H. Matsuoka et al., submitted.

Proximity induced spin-orbit coupling and magnetism in graphene

Alexey Kaverzin

With a reference to our experimental observations I will discuss how proximity effects modify the spin transport phenomena in graphene when it is placed in the vicinity of other layered materials. For example, the combination of graphene and TMDs results in the presence of large spin-orbit interaction imprinted from TMD into graphene with the emergence of spin manipulation mechanisms including conversion between spin and charge currents. I will highlight our recent results obtained on a van der Waals heterostructure of graphene and anti-ferromagnetic material CrSBr. The presence of CrSBr introduces a large exchange interaction in graphene such that its conductivity becomes spin polarised with the polarisation of approximately 14%. This implies that spin current is generated in graphene on CrSBr with efficiency close to that of the conventional ferromagnetic materials. Overall, we experimentally demonstrate the functionality of various building blocks that can be used for assembly of spin-based devices made out of layered materials only.

Electrostatic Control of Magnetism in Van Der Waals Ferromagnets

Ivan Verzhbitskiy

Control of magnetism via electric fields is a long-standing exciting challenge of fundamental significance for future spintronic devices. Recent discovery of two-dimensional magnetism in van der Waals systems such as CrI3, Fe3GeTe2, and Cr2Ge2Te6 (CGT) highlights their unique potential as a platform to probe the interplay between charge and magnetic ordering [1]. Here, we report the first observation of carrier-induced ferromagnetic order in heavily doped thin crystals of CGT [2]. Upon degenerate electron doping, the CGT transistor exhibits clear hysteresis in the magnetoresistance (MR), which is a distinctive signature of ferromagnetism. Surprisingly, the hysteresis persists up to 200 K, which is in contrast to undoped CGT whose Curie temperature is only 61 K. We demonstrate that the Curie temperature can be modulated over 140 K by altering the electron density. Further, we find the magnetic easy-axis of doped CGT to lie within the plane of the crystal. This is in stark contrast to the out-of-plane magnetic easy-axis of the pristine CGT. We attribute these changes to emergence of the double-exchange interaction mediated by free carriers. This mechanism dominates over superexchange interaction, which is responsible for the ferromagnetic order in undoped CGT. Our calculations show that the magnetic anisotropy energy changes sign in degenerate doping limit, in agreement with our experimental observations. Our findings reveal a unique role of the electric field in tailoring the magnetic anisotropy and leading exchange interaction in semiconducting 2D ferromagnets.

[1] Gibertini, M.; Koperski, M.; Morpurgo, A. F. & Novoselov, K. S. Magnetic 2D materials and heterostructures. Nat. Nanotechnol. 14, 408–419 (2019).

[2] Verzhbitskiy, I.; Kurebayashi, H.; Cheng, H.; Zhou, J.; Khan, S.; Feng, Y. P. & Eda, G. Controlling the magnetic anisotropy in Cr2Ge2Te6 by electrostatic gating. Nat. Electron. (2020), DOI:https://doi.org/10.1038/s41928-020-0427-7

On-line SPICE-SPIN+X Seminars

On-line Seminar: 29 July 2020 - 15:00 (CET)

Macroscopic magnonic quantum states

Burkard Hillebrands, Technische Universität Kaiserslautern

Finding new ways for fast and efficient processing and transfer of data is one the most challenging tasks nowadays. Elementary spin excitations ‒ magnons (spin wave quanta) ‒ open up very promising directions of high-speed and low-power information processing.
Magnons are bosons, and thus they can spontaneously form a spatially extended coherent ground state ‒ a Bose-Einstein condensate (BEC) – which can be established independently of the magnon excitation mechanism even at room temperature. An extraordinary challenge is the use of macroscopic quantum phenomena such as the magnon BEC for the information transfer and processing.
Very promising is the use of magnon supercurrents driven by a phase gradient in the magnon BEC. Imposing such a phase gradient onto the BEC’s wave function we have found using Brillouin light scattering spectroscopy that local heating by a probing laser beam leads to an excessive decay of the freely evolving magnon BEC. This is a fingerprint of the supercurrent efflux of condensed magnons. Moreover, we revealed that the condensed magnons being pushed out from the heated area form compact density humps, which propagate over long distances through the thermally homogeneous magnetic medium. We refer to them as a superposition of Bogoliubov waves with oscillations of both the amplitude and the phase of the magnon BEC’s wave function. In the long-wavelength limit, these waves have a linear dispersion law and can be considered as a magnon second sound potentially featuring viscosity-free propagation.
A further consequence of a magnon BEC is the prediction of the existence of a magnon ac Josephson effect. Recently, we discovered this effect in a room-temperature magnon BEC. The magnon condensate was prepared in a parametrically populated magnon gas around a potential trench created by a dc electric current. The appearance of the magnonic Josephson effect is manifested by oscillations of the magnon BEC density in the trench, caused by a coherent phase shift between magnon condensates from the left and right zones of the trench.

 

PDF file of the talk available here

 

 

A perspective on the synthesis and modifications of 2D transition metal dichalcogenides by vacuum methods

Matthias Batzill

 

In this tutorial talk, I am introducing the concept of van der Waals epitaxy of transition metal dichalcogenides (TMDs) and the endeavor of finding potentially ferromagnetic 2D materials. Epitaxial mono- or few-layer films allow detailed measurement of electronic structure by angle resolved photoemission and thus determine layer dependent properties and the role of interlayer interactions of the properties. In addition, scanning tunneling microscopy can give information on the growth process and defect structures in the films. We discuss selected cases of TMDs. For VSe2 we suggest a competition between charge density and ferromagnetic ordering for the ground state. While in CrTe2 the ground state may be the semiconducting 1H-phase rather than the sought metallic and possibly ferromagnetic 1T-phase. Formation of ultrathin intercalation compounds are also discussed as a potential ultrathin ferromagnets. Finally, we discuss properties of defects in TMDs and how these may help in inducing magnetic properties. The incorporation of magnetic dopants may be one approach and recent reports suggest the possibility of diluted ferromagnetic 2D semiconductors. While there are many unanswered questions, a controlled vacuum synthesis and characterization of monolayer materials is an important aspect to find new materials.

Graphene-based van der Waals heterostructures for Spintronics

Juan F. Sierra

In recent years, spin-based technologies, in which information is carried by spin instead of charge, have become promising for “beyond-CMOS” devices. Graphene and other two dimensional materials have rapidly established themselves as intriguing building blocks for spintronics applications [1]. Because of the graphene intrinsic low spin-orbit interaction, spins can flow snugly through its crystal lattice over long distances, resulting in an ideal spin channel. At the same time, the graphene’s low spin-orbit interaction inhibits the manipulation of spins, which is the cornerstone for successfully implementing spin-based devices. Nevertheless, this bottleneck can be overcome by combing graphene with other layered materials in artificial van der Waals heterostructures. In this talk, I will present a set of experiments where we study the spin-relaxation in graphene-transition metal dichalcogenides heterostructures [2]. In such van der Waals systems, spin-orbit coupling in graphene is enhanced by proximity effects. As a consequence, the spin dynamics becomes anisotropic [2, 3], with a spin relaxation that depends on the spin orientation. Furthermore, we demonstrate an efficient spin-charge interconversion driven by the Spin Hall effect and inverse spin galvanic effect at room temperature [4].
1. W. Han et al., Nature Nanotechnology 9, 794 (2014).
2. L. A. Benítez, J. F. Sierra et al., Nature Physics 14, 303 (2018).
3. L. A. Benítez, J. F. Sierra et al., APL Materials 7, 120701 (2019).
4. L. A. Benítez, W. Savero Torres, J. F. Sierra, et al., Nature Materials 19, 170 (2020).

On-line SPICE-SPIN+X Seminars

On-line Seminar: 22 July 2020 - 15:00 (CET)

Transversal transport coefficients and topological properties

Ingrid Mertig, Martin Luther University Halle-Wittenberg, Germany

Spintronics is an emerging field in which both charge and spin degrees of freedom of electrons are utilized for transport. Most of the spintronic effects—like giant and tunnel magnetoresistance—are based on spin- polarized currents which show up in magnetic materials; these are already widely used in information technology and in data storage devices.
The next generation of spintronic effects is based on spin currents which occur in metals as well as in insulators, in particular in topologically nontrivial materials. Spin currents are a response to an external stimulus—for example electric field or temperature gradient—and they are always related to the spin-orbit interaction. They offer the possibility for future low energy consumption electronics.
The talk will present a unified picture, based on topological properties, of a whole zoo of transversal transport coefficients: the trio of Hall, Nernst, and quantum Hall effects, all in their conventional, anomalous, and spin flavour. The formation of transversal charge and spin currents and their interconversion as response to longitudinal gradients is discussed.

PDF file of the talk available here

New Developments on Chromium Trihalides 2D Ferromagnets

David Soriano

The discovery of 2D ferromagnets in 2017 has opened new ways to explore novel physical phenomena at the nanoscale. In the first part of my talk, I will briefly discuss the recent advances in chromium trihalides, from fundamentals to applications.[1] In the second part, I will focus on our recent work regarding the role of Coulomb interactions in the intralayer exchange, the electrical tunability of interlayer magnetism in bilayer CrI3,[2] and the exchange proximity effects in van der Waals heterostructures containing chromium trihalides.[3,4] [1] Magnetic Two-Dimensional Chromium Trihalides: A Theoretical Perspective. D. Soriano, M. I. Katsnelson, and J. Fernández-Rossier. Submitted to Nano Letters.

[2] Magnetic polaron and antiferromagnetic-ferromagnetic transition in doped bilayer CrI3. D. Soriano, and M. I. Katsnelson. Phys. Rev. B 101, 041402(R) (2020)

[3] Van der Waals Spin Valves. C. Cardoso, N. A. García-Martínez, and J. Fernández-Rossier. Phys. Rev. Lett. 121, 067701 (2018)

[4] Exchange-bias controlled correlations in magnetically encapsulated twisted van der Waals dichalcogenides. D. Soriano, and J. L. Lado. arXiv:2006.09953

van der Waals layered magnetic semiconductors

Young Hee Lee

 

The ferromagnetic state in van der Waals two-dimensional (2D) materials has been reported recently in the monolayer limit. Intrinsic CrI3 and CrGeTe3 semiconductors reveal ferromagnetism but the Tc is still low below 60K. In contrast, monolayer VSe2 is ferromagnetic metal with Tc above room temperature but incapable of controlling its carrier density. Moreover, the long-range ferromagnetic order in doped diluted chalcogenide semiconductors has not been demonstrated at room temperature. The key research target is to realize the long-range order ferromagnetism, Tc over room temperature, and semiconductor with gate tunability. Here, Ferromagnetic order is manifested using magnetic force microscopy up to 360K, while retaining high on/off current ratio of ~105 at 0.1% V-doping concentration. The V-substitution to W siteskeep a V-V separation distance of 5 nm without V-V aggregation, scrutinized by high-resolution scanning transmission-electron-microscopy. More importantly, the ferromagnetic order is clearly modulated by applying a back gate. We also observe a ferromagnetic hysteresis loop together with oscillatory behavior at room temperature in diluted V-doped WSe2, while maintaining the semiconducting characteristic of WSe2 with a high on/off current ratio of five orders of magnitude. Our findings open new opportunities for using two-dimensional transition metal dichalcogenides for future spintronics.