News and posts

09.12.2019 – Elastic Tuning and Response of Electronic Order

Elastic Tuning and Response of Electronic Order

New physical phenomena have emerged from a particularly strong coupling between a materials’ elasticity and its symmetry-broken electronic quantum phases. Examples are reversible superelasticity with large recoverable strain in iron-based materials, strong nonlinear elastic response with violation of Hooke’s law and critical elasticity in pressurized organic charge-transfer salts, a doubling of the superconducting transition temperature in strained strontium ruthenate, strain-induced charge order in cuprate superconductors, as well as nematicity in iron-based superconductors. Static and dynamic strain manipulation has emerged as a new knob to tune and shape a material’s electronic properties.

For videos of the talks and further information, please visit the workshop home page.

Posted on | Posted in News

Program - Elastic Tuning and Response of Electronic Order

 

 

 

 

Monday, December 9th

Morning Session 

08:50 – 09:20 Registration
09:20 – 09:30 Opening Remarks
09:30 – 10:20 Ian FISHER, Stanford University
Feeling the strain: tuning the critical temperature of electronic nematic phases
10:30 – 10:50 Coffee Break
10:50 – 11:20 Anna BÖHMER, KIT
Tuning magnetism in iron-based superconductors
11:30 – 12:00 Bernd BÜCHNER, IFW
Strain dependent transport and nematicity in Fe based superconductors
12:00 – 14:30 Lunch Break

Afternoon Session

14:40 – 15:10 Elena GATI, IOWA State University
Effect of hydrostatic pressure and uniaxial stress on the competing phases in iron-based superconductors
15:20 – 15:50 Suguru HOSOI, Osaka University
Elastoresistance measurements in nematic superconductors
16:00 – 16:30 Collin BROHOLM, Johns Hopkins University
Magneto-elasticity in Fragile Magnets
18:00 – 19:30 Dinner

Tuesday, December 10th

Morning Session

09:00 – 09:50 Steven Allan KIVELSON, Stanford University
Nematicity, strain, and disorder: Universal features from statistical mechanics
10:00 – 10:30 Heejae KIM, Max Planck Institute for Polymer Research
Nonlinear spectroscopic study of electron-phonon coupling
10:30 – 10:50 Coffee Break & Poster Session
10:50 – 11:20 Rafael FERNANDES, University of Minnesota
Contrasting nematicity in rigid lattices and moiré superlattices
11:30 – 12:00 Kristin KLIEMT, University Frankfurt
Advanced methods for single crystal growth of Eu- and Yb-based intermetallic systems
12:00 – 14:30 Lunch Break & Poster Session

Afternoon Session

14:30 – 15:00 Stephen ROWLEY, Cambridge
Strong electron pairing in ferroelectric superconductors
15:10 – 15:40 Philipp GEGENWART, University of Augsburg
Thermal expansion signatures of the quadrupolar Kondo effect
15:50 – 16:20 Marcel SCHRODIN, KIT
Nanoscale sensing with single spins in diamond
16:20 – 17:30 Poster Session
18:00 – 19:30 Dinner

Wednesday, December 11th

Morning Session

09:00 – 09:50 Michael LANG, University of Frankfurt
Molecular metals – test ground for correlated electrons in a compressible lattice
10:00 – 10:30 Clifford HICKS, MPG
Superconductors and magnets under uniaxial stress
10:30 – 10:50 Coffee Break 
10:50 – 11:20 Helen GOMONAY, JGU
Elastic manipulation of antiferromagnetic domain structure
11:30 – 12:00 Kristin WILLA, KIT
Evidence for nematic superconductivity in the superconducting doped topological insulators NbxBi2Se3 and SrxBi2Se3
12:00 – 14:30 Lunch 

Afternoon Session 

14:30 – 15:00 Stuart BROWN, UCLA
Unconventional superconductivity in Sr2RuO4, probed under stressed conditions
15:10 – 15:40 Taner YILDIRIM, NIST
Pressure and Strain Control of Crystal Symmetry, Fermi Surface Reconstruction and Superconductivity in Weyl semimetal MoTe2
15:50 – 16:00 Closing Remarks

 

Posted on | Posted in Allgemein

12.11.2019 – Novel Electronic and Magnetic Phases in Correlated Spin-Orbit Coupled Oxides

Novel Electronic and Magnetic Phases in Correlated Spin-Orbit Coupled Oxides

The interplay between spin, orbit and electron correlation has emerged as a new paradigm in contemporary condensed matter physics and represents a rich playground for the realization of novel quantum state of matters with exotic electronic and magnetic properties including Dirac-Mott insulators, Lifshitz/Slater phases, Multipolar and Kitaev model magnetism, unconventional superconductivity and topological physics.

For videos of the talks and further information, please visit the workshop home page.

Posted on | Posted in News

15.10.2019 – Molecular Electro-Opto-Spintronics

Molecular Electro-Opto-Spintronics

Molecular electronics originally promised miniaturization of molecular devices using Nature’s smallest building blocks to allow for novel electronic function by simply altering the chemical structure of the molecular component. Molecular electronics has evolved towards a complementary technology to silicon-based electronics, providing functionalities not possible with classical electronic devices. After more than 40 years of experiments, it remains a challenge to rationally design molecule-electrode junctions due the complex interplay between electronic structure and the chemical/supramolecular arrangement of the interfaces. Unlike traditional CMOS electronics, comprehensive design rules for molecular junctions are not available yet. Only bits and pieces have been published scattered across disciplines, including interface engineering, supramolecular chemistry, surface science, computational science, physics, chemistry, optics, biology and micro/nanofabrication.

For videos of the talks and further information, please visit the workshop home page.

Posted on | Posted in News

07.10.2019 – Antiferromagnetic Spintronics: from topology to neuromorphic computing

Antiferromagnetic Spintronics: from topology to neuromorphic computing

The new field of antiferromagnetic spintronics focuses on making antiferromagnets active elements of spintronic devices. The higher complexity of the ordered phase and parameter space in antiferromagnets have given rise to new avenues of basic research that range from topological quasiparticle dynamic manipulation, multipole order effects, ultra-fast dynamics, and even applications towards neuromorphic computing and IoT.

The new field is of interest to the strongly correlated effects community and the community focused on topological matter. It has connected to the current ferromagnetic spintronics research by creating entirely new ways of rethinking spin phenomena in antiferromagnets, while benefiting from the pioneering works in antiferromagnetic materials.

For videos of the talks and further information, please visit the workshop home page.

Posted on | Posted in News

30.09.2019 – Young Research Leader Group Workshop: Topomagnetism Is Coming: Relativity and Correlations in Topological Magnets

YRLGW: Topomagnetism Is Coming: Relativity and Correlations in Topological Magnets

Remarkable advances in strongly correlated and relativistic condensed matter physics have been made over the past decade by these largely non-interacting communities. Interestingly, their attention recently focused on the same grand challenges such as room-temperature quantum chiral edge modes, topological superconductivity, or topological computation.

The research of nonmagnetic materials culminated in predicting that approximately one third of them exhibit topological electronic structure. In contrast, the investigation of topological magnets is progressing at much slower pace albeit time-reversal symmetry broken topological phases demand magnetic order. For a long time, low-dimensional topological systems were anticipated to be naturally incompatible with robust magnetism. However, recent theoretical and experimental efforts have revealed low-dimensional as well as 3D topological insulators and Weyl semimetal magnets. The relativistic phenomena, e.g. the spin Hall, quantum spin Hall, or magnetic spin-Hall effect, were originally predicted within the single-particle picture. However, realistic predictions of magnetic materials, requires inclusion of the electronic correlations. Conversely, the correct description of strongly correlated magnets with high atomic numbers needs to include spin-orbit coupling phenomena.

For videos of the talks and further information, please visit the workshop home page.

Posted on | Posted in News

Non-Abelian band topology in non-interacting metals

Tomáš Bzdušek

Stanford University

We show that non-Abelian topological structure arises inside the momentum space of semimetals and metals under various symmetry settings [1], including PT-symmetric systems with negligible spin-orbit coupling, and C2T-symmetric systems with or without spin-orbit coupling. This results in non-Abelian topological charges of band-structure nodes, similar to those that describe disclinations in biaxial nematics, implying non-trivial braiding phenomena inside the momentum space [2]. We discuss how the non-Abelian band topology can be captured using various mathematical techniques, including homotopy groups, characteristic classes, and Wilson-loop Pfaffians [3]. We conclude the talk by briefly commenting on the interplay of this newly discovered topological structure with space-group symmetry.

[1] Q.S. Wu, A. A. Soluyanov, T. Bzdušek, arXiv:1808.07469 (2018)
[2] A. Tiwari and T. Bzdušek, arXiv:1903.00018 (2019)
[3] A. Bouhon, R.-J. Slager, T. Bzdušek, arXiv:1907.10611 (2019)

Skyrmion Crystals as Topological Magnonics Platforms

Sebastián A. Díaz

Department of Physics, University of Basel, Basel, Switzerland

The quest to harness magnonic spin waves, aided by insights from topological matter, has
led to the emergence of the new field of topological magnonics. Among the systems that have
been predicted to support topologically protected magnonic edge states are spatially periodic
noncollinear textures. A noteworthy example are skyrmion crystals, which have garnered
much interest lately due to their topological transport properties and the potential to use
skyrmions as information carriers in future high-density, low-power storage and logic
devices. In this talk I will discuss our latest findings on topologically protected magnonic
edge states in antiferromagnetic as well as ferromagnetic skyrmion crystals.

Magnon spin transport in antiferromagnets

Romain Lebrun(1), Andrew Ross(1,2), Asaf Kay(3), David Ellis(3), Daniel Grave(3), O. Gomonay(1,2,) Lorenzo Baldrati(1), Alireza Qaiumzedah(4), Camilo Ulloa(5), J. Sinova(1,2), Arne Brataas(4), Avner Rothschild(3), Rembert Duine(4,5,6) and Mathias Kläui(1,2,3,4)

1 Institute for Physics, Johannes Gutenberg University Mainz, D-55128 Mainz, Germany
2 Graduate School of Excellence Material Science in Mainz, Staudingerweg 9, 55128, Mainz, Germany
3 Department of Materials Science and Engineering, Technion-Israel Institute of Technology
4 Center for Quantum Spintronics, Norwegian University of Science and Technology, NO-7491 Trondheim, Norway
5 Utrecht University, Princetonplein 5, 3584 CC Utrecht, Netherlands
6 Department of Applied Physics, Eindhoven University of Technology, P.O. Box 513, 5600 MB Eindhoven, The Netherlands

In contrast to ferromagnets, antiferromagnets benefit from unparalleled stability with respect to applied external fields, magnetization dynamics at THz frequencies and a lack of stray fields [1]-[2]. Many theoretical studies have been undertaken describing the mechanisms through which antiferromagnets could allow for the propagation of spin current across the long distances which would be required for integration into information transfer and logic devices [3]-[4]. Recently, we demonstrated that in antiferromagnetic insulators, a diffusive magnonic spin current is able to propagate over tens of micrometers carried by the intrinsic Néel order using a single crystal of the most common insulating antiferromagnet, hematite (α-Fe2O3)[5]. With low damping and characteristic frequencies of hundreds of GHz, this compound allows for antiferromagnetic spin-waves to propagate as far as in YIG, a ferromagnetic material with the lowest known damping that is the material of choice for magnonic devices. Through measurements of the spin Hall magnetoresistance, the internal crystal anisotropies can be extracted [6], allowing for a precise determination of critical fields without the need for high frequency resonance experiments.
Here, we grow high quality antiferromagnetic thin films of hematite (< 500 nm) and show that they can also allow pure magnonic current to propagate over long-distances, opening the way towards a development and an integration of antiferromagnetic magnonic devices. We then discuss the role of the growth orientation and of the magnetic fields required to induce transport. By controlling the antiferromagnetic domains, we demonstrate how magnetic textures impact the propagation of polarized magnons [7]. Finally, we discuss the temperature dependence of the magnon propagation for magnons originating from an electrical spin-bias at the interface of hematite and platinum or from thermal heating of the hematite layer, and demonstrate that one can even achieve zero-field, room temperature magnon transport in insulating antiferromagnets.

[1] T. Jungwirth et al., Nat. Phys. 14, 200-203 (2018)
[2] V. Baltz et al., Rev. Mod. Phys. 90, 015005 (2018)
[3] S. Takei et al., Phys. Rev. B, 90, 94408 (2014)
[4] S. Bender et al., Phys. Rev. Lett. 19, 056804 (2017)
[5] R. Lebrun et al., Nature 561, 222-225 (2018)
[6] R. Lebrun et al., Communications Physics 2 50 (2019)
[7] A. Ross et al., arXiv:1907.02751 (2019)

Boundary Obstructed Topological Phases

Raquel QUEIROZ

Weizmann Institute of Science

Symmetry protected topological (SPT) phases are gapped phases of matter that cannot be deformed to a trivial phase without breaking the symmetry or closing the bulk gap. In this talk I will introduce a new notion of a topological obstruction that is not captured by bulk energy gap closings in periodic boundary conditions. More specifically, we say two bulk Hamiltonians belong to distinct boundary obstructed topological `phases' (BOTPs) if they can be deformed to each other on a system with periodic boundaries, but cannot be deformed to each other for symmetric open boundaries without closing the gap at at least one high symmetry region on the surface. I will discuss the double-mirror quadrupole model [Science, 357(6346), 2018] and a dimerized weak topological insulator [arxiv 1809.03518] as examples of BOTPs. I will describe the general framework to study boundary obstructions in free-fermion systems in terms of Wannier band representations (WBR), an extension of the recently-developed band representation formalism to Wannier bands. WBRs capture the notion of topological obstructions in the Wannier bands which can then be used to study topological obstructions in the boundary spectrum by means of the correspondence between the Wannier and boundary spectra. This establishes a form of bulk-boundary correspondence for BOTPs by relating the bulk band representation to the boundary topology.