Szemináriumok

Ab initio study of weakly ferromagnetic antiferromagnets

Időpont: 
2021. 05. 01. 10:15
Hely: 
online (Teams)
Előadó: 
András Deák (BME)
Antiferromagnets have lately appeared in the forefront of spintronics research. Collinear insulating antiferromagnets have exciting applications in magnonic spin transport, while noncollinear antiferromagnets can show for instance anomalous Hall effect or magnon-magnon scattering. In the talk we will detail our investigations of two distinct systems: the noncollinear antiferromagnet family Mn3Z with Z=Sn, Ge and Ga [1]; and hematite (alpha-Fe2O3), a well-known collinear insulating antiferromagnet showing weak ferromagnetism. We use a multiscale description by computing spin model parameters from first principles and assessing the ground state spin configuration and its stability using this model. With this approach we can tackle the nature of the weak ferromagnetic distortion in these antiferromagnets, and provide spin model parameters that can be used in large-scale simulations of magnon dynamics effects.
 
[1]: B Nyári, A Deák, L Szunyogh, Phys. Rev. B 100, 144412 (2019)

Time dependent electric transport in nodal loop semimetals

Időpont: 
2021. 05. 07. 10:15
Hely: 
online (Teams)
Előadó: 
Zoltán Okvátovity (BME)

Close to the Fermi energy, nodal loop semimetals have a torus-shaped, strongly anisotropic Fermi surface which affects their transport properties. Here we investigate the non-equilibrium dynamics of nodal loop semimetals by going beyond linear response and determine the time evolution of the current after switching on a homogeneous electric field. The current grows monotonically with time for electric fields perpendicular to the nodal loop plane, however, it exhibits non-monotonical behavior for field orientations aligned within the plane. After an initial non-universal growth ~Et, the current first reaches a plateau ~E. Then, for perpendicular directions, it increases while for in-plane directions it decreases with time to another plateau, still ~E. These features arise from interband processes. For long times or strong electric fields, the current grows as ~E^(3/2)t or ~E^3t^2 for perpendicular or parallel electric fields, respectively. This non-linear response represents an intraband effect where the large number of excited quasiparticles responds to the electric field. Our analytical results are benchmarked by the numerical evaluation of the current from continuum and tight-binding models of nodal loop semimetals.

 
Manuscript: Z. Okvatovity, L. Oroszlany, B. Dora, arXiv:2104.07632)

Excitons in twisted flatland

Időpont: 
2021. 05. 10. 14:15
Hely: 
online (Teams)
Előadó: 
You Zhou (Maryland)

Atomically thin transition metal dichalcogenides (TMDs) have attracted recent interest due to their unique excitonic properties. Lateral confinement of excitons to generate two-dimensional exciton arrays may open up new avenues for quantum optoelectronics such as topological photonics and quantum emitter arrays. Realizing such emitter arrays, however, requires the development of new methods to engineer the excitonic energy landscape at the nanoscale. In this talk, I will focus on how to use twisted TMD bilayers to engineer the coherence and relaxation properties of excitons. I will discuss lattice reconstruction effects in the moiré pattern and correlating their importance in determining the excitonic behaviors. Finally I will discuss prospects of realizing tunable exciton arrays in twisted heterostructures for exploring novel optoelectronics and many-body states.

Topological Weaire-Thorpe models of amorphous matter

Időpont: 
2021. 05. 21. 10:15
Hely: 
online (Teams)
Előadó: 
Dániel Varjas (Stockholm)
Amorphous solids remain outside of the classification and systematic discovery of new topological materials, partially due to the lack of realistic models that are analytically tractable. Here we introduce the topological Weaire-Thorpe class of models, which are defined on amorphous lattices with fixed coordination number, a realistic feature of covalently bonded amorphous solids. Their short-range properties allow us to analytically predict spectral gaps. Their symmetry under permutation of orbitals allows us to analytically compute topological phase diagrams, which determine quantized observables like circular dichroism, by introducing symmetry indicators for the first time in amorphous systems. These models and our procedures to define invariants are generalizable to higher coordination number and dimensions, opening a route towards a complete classification of amorphous topological states in real space using quasilocal properties.
 
 
Publication: Q Marsal, D Varjas, AG Grushin: Topological Weaire-Thorpe models of amorphous matter, Proc. Natl. Acad. Sci., 202007384 (2020)

Symmetry-enforced band topologies in metals and magnets

Időpont: 
2021. 05. 31. 14:15
Hely: 
online (Teams)
Előadó: 
Andreas Schnyder (Stuttgart)
In this talk, I will survey recent developments regarding the topological classification of symmetry-enforced band topologies in (semi)metals and magnets. These topological properties of the band structure are enforced to exist by symmetry alone, independent of the band dispersion, orbital content, and chemical composition of the material [1]. Hence, once the space group symmetries that enforce the desired band topologies have been identified, a suitable material can be found simply by browsing materials databases by space group numbers [2-4]. In this way, we have identified, among others [2-5], the topological materials ZrIrSn [2] and ferromagnetic MnSi [5], which will be discuss in detail.
 
The material ZrIrSn exhibits Weyl nodal lines near the Fermi energy, whose existence is guaranteed by a glide mirror symmetry. The topology of this nodal line is characterized by a quantized Pi-Berry phase, which leads to drumhead surface states. Ferromagnetic MnSi, on the other hand, has topological nodal planes on the BZ boundary, which are enforced by a combination of time-reversal with screw rotation symmetries. These nodal planes are sources of Berry flux, which is absorbed by single Weyl points at the center of the BZ. We discuss experimental consequences of these nodal planes in the surface spectra and de Haas-van Alphen measurements [5]. 
 
[1] Y. Zhao, A. Schnyder, Phys. Rev. B 94, 195109 (2016)
[2] J. Zhang, Y. Chan, C. Chiu, M. Vergniory, L. Schoop, A. Schnyder, Phys. Rev. Materials 2, 074201 (2018) 
[3] Y. Chan, B. Kilic, M. Hirschmann, C. Chiu, L. Schoop, D. Joshi, A. Schnyder, Phys. Rev. Materials 3, 124204 (2019)
[4] M. Hirschmann, A. Leonhardt, B. Kilic, D. Fabini, A. Schnyder, arXiv:2102.04134
[5] M. Wilde, M. Dodenhöft, A. Niedermayr, A. Bauer, C. Pfleiderer, to appear in Nature

Mean Field Approximation for solving QUBO problems

Időpont: 
2021. 09. 10. 10:15
Hely: 
online (Teams)
Előadó: 
Máté Veszeli (ELTE)
Mean Field Approximation for solving QUBO problems
 
Optimization is one of the most useful mathematical tools in everyday life. The Quadratic Unconstrained Binary Optimization (QUBO) problem is a ubiquitous, NP hard problem, with no efficient solution, but many good approximations (simulated annealing, coherent Ising machine, etc). An adiabatic quantum computer would be perfect for this task, but its physical implementation is cumbersome, as the system can't be separated from its environment, and a large number of qubits would be needed.
I will present a mean-field-based algorithm we developed[1], imitating quantum annealing, to solve the QUBO problem, and compare it with mean field approximation as familiar from statistical physics.
 
[1]:  MT Veszeli, G Vattay: https://arxiv.org/abs/2106.03238

Classical Theory of Universal Quantum Work Distribution in Chaotic Fermi Liquids

Időpont: 
2021. 09. 17. 10:15
Hely: 
online (Teams)
Előadó: 
András Grabarits (BME)
We present [1] a universal theory of quantum work statistics in generic chaotic, disordered Fermi liquid systems within a driven random matrix formalism. By extending P. W. Anderson’s orthogonality determinant formula to compute quantum work distribution, we find that work statistics is non-Gaussian and is characterized by a few dimensionless parameters. At longer times, quantum interference effects become irrelevant and the quantum work distribution is well-described in terms of a purely classical ladder model with a symmetric exclusion process in energy space, while bosonization and mean field methods provide accurate analytical expressions for the work statistics. Our random matrix and mean field predictions are validated by numerical simulations for a two-dimensional disordered quantum dot, and can be verified by calorimetric measurements on nanoscale circuits.
 
[1]:  A Grabarits, M Kormos, I Lovas, G Zaránd: arXiv:2107.10245

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