Zeit Sprecher & Vortragsthema
Mi 11:00
Hybrid Zoom / CN B.425 R.206
Hilary Noad
Max-Planck-Institut für Chemische Physik fester Stoffe, Dresden
Probing the interplay between electronic systems and the lattice in transition metal oxides

A central theme in the modern study of quantum materials is the coupling between magnetic or electronic order and the underlying crystal lattice. Probing this interplay using conventional thermodynamic or transport measurements can be onerous, often requiring the measurement of series of samples that vary, for example, epitaxial strain, isovalent substitution, or isotopic abundance to realize a range of lattice parameters while leaving the chemical nature of the material intact. In this talk, I will describe two novel approaches to studying the coupling between structural and electronic degrees of freedom, first by locally resolving the intrinsic variation of strain within a sample, and then by in situ control of the global strain field. In the first part of my talk, I will discuss how I used a local magnetic probe, scanning superconducting quantum interference device (SQUID) microscopy, to study the influence of the intrinsic twin structure on superconductivity in heterostructures based on strontium titanate (SrTiO3). In the second part, I will present measurements of the stress-strain relation of bulk strontium ruthenate (Sr2RuO4) under uniaxial pressure, revealing a large lattice softening as the material undergoes a Lifshitz transition. These studies demonstrate the utility of novel approaches in revealing the critical role that the lattice plays in the ordered phases of quantum materials

Di 16:00
Hybrid Zoom / CN B.425 R.206
David Larbalestier
Mechanical Engineering Applied Superconductivity Center and Florida State UniversityTallahassee, Florida, USA
Understanding the real, imperfect nature of REBCO (REBa2Cu3Ox with RE=Rare Earth elements) coated conductors and its implications for ultra-high magnetic field used

Mi 11:00
Hybrid Zoom / CN B.425 R.206
Jürgen Lisenfeld
Karlsruher Institut für Technologie - Physikalisches Institut
Studying atomic tunneling systems with superconducting qubits

At low temperatures, practically all amorphous materials show a variety of anomalous properties. These are believed to arise from structural material defects forming two-level quantum systems (TLS) which can interact with photons and phonons. However, despite 50 years of active research, a thorough understanding of the nature of TLS has remained elusive.
With the advent of superconducting quantum circuits, new tools became available for the study of TLS. By exploiting the fragility of the circuit's coherent quantum state, it is now possible to resolve and characterize even single TLS defects.
After a brief review of the physics of TLS defects and the limitations of the standard tunneling model, I will present our experiments where we use superconducting qubits as interfaces to single defects. A focus lies on techniques to tune TLS defects by applied mechanical strain or electric fields, which have proven useful to reveal the TLS' positions and their interactions with other TLS, phonons, and quasiparticles. Such new insights may become especially valuable since TLS defects have a widespread importance as a source of noise that affects various devices.

Mi 11:00
Hybrid Zoom / CN B.425 R.206
Yixi Su
Jülich Centre for Neutron Science JCNS at MLZ, Forschungszentrum Jülich
Neutron scattering on magnetic topological materials

Magnetic topological materials, such as magnetic Dirac and Weyl semimetals, and intrinsic magnetic topological insulators, in which topologically non-trivial band structures, magnetism and electronic correlation effects can be intertwined, have recently emerged as an exciting platform to explore exotic states and novel functionalities. As a unique microscopic probe for magnetism, neutron scattering is ideally suited for the investigations of magnetic correlations over a wide range of length and time scales in these emergent quantum materials. In this talk, I will present our recent neutron scattering studies of magnetic topological materials, with the main aim to demonstrate the fascinating interplay between topology, magnetism and electronic correlation. In the Dirac semimetal EuMnBi2, the evidence for the possible impact of magnetism on Dirac fermions is obtained via a detailed neutron diffraction study of the spin-flop transition [1]. In the two-dimensional van der Waals honeycomb ferromagnets CrSiTe3 and CrGeTe3, the exotic topological magnon insulators, the bosonic analogue of topological insulators, have been experimentally realized based on our inelastic neutron scattering study and theoretical analysis of spin-wave excitations [2]. Furthermore, in the magnetic Weyl semimetal Mn3Sn, an unusual magnetic phase transition that is driven by emergent many-body effects can be revealed via our combined polarised neutron scattering study and band-structure calculations [3].
[1] F. Zhu et al., Phys. Rev. Research 2, 043100 (2020)
[2] F. Zhu et al., Sci. Adv. 7, eabi7532 (2021)
[3] X. Wang et al., (submitted).

Mi 15:00
Hybrid Zoom / CN B.425 R.206
Christos Panagopoulos
Nanyang Technological University, Singapore
Chirality Engineering in Quantum Matter

Quantum geometry manifests itself in a plethora of materials and architectures including topological insulators, Archimedean magnets, Weyl/Dirac semimetals, transition metal oxides and dichalcogenides, and can also be engineered via interaction with electromagnetic fields. The emergent internal structure can radically alter our understanding of quantum mechanical wavefunctions of charge carriers and quasiparticles, yielding modular transport, optical, magnetic responses that are critically interlinked. I will introduce our efforts to geometrically tune the microscopic interactions responsible for macroscopic quantum coherences, through two recent examples. Namely, the first architecture in which superconductivity and magnetism interact via distinct topological solitons and a novel physical qubit platform based on the energy-level quantization of the helicity degree of freedom.

Mi 11:00
Hybrid Zoom / CN B.425 R.206
The role of synthesis experts in quantum materials and technology research

High-quality crystals are required for experiments in solid state physics and also industrial research fields. Such crystals are often synthesized by experts (as known as sample growers). They also study physical properties of materials and conduct joint research with other researchers for further study and even for mass production. However, the work of synthesis experts is in some ways unknown to physicists. Based on my experience studying superconductors [1, 2], magnetic memory materials [3], and battery materials in academia and industry, I will introduce and explain this aspect to researchers and students.
[1] N. H. Sung, C. J. Roh, K. S. Kim, and B. K. Cho, Possible multigap superconductivity and magnetism in single crystals of superconducting La2Pt3Ge5 and Pr2Pt3Ge5, Phys. Rev. B 86, 224507 (2012)
[2] Y. K. Kim, N. H. Sung, J. D. Denlinger, B. J. Kim, Observation of a d-wave gap in electron-doped Sr2IrO4, Nature Physics 12, 37 (2016)
[3] N. H. Sung, F. Ronning, J. D. Thompson, and E. D. Bauer, Magnetic phase dependence of the anomalous Hall effect in Mn3Sn single crystals, Appl. Phys. Lett. 112, 132406 (2018)

Mi 11:00
Hybrid Zoom / CN B.425 R.206
Synthesis and characterization of Ba1-xCaxNi2As2 with thermodynamic, transport and spectroscopic methods

In many unconventional superconductors, new types of exotic electronic orders are often found in proximity to the superconducting phase. These can consist in charge density waves, various types of magnetic orders or electronic nematicity. In many cases, the nature of the interplay between these orders and superconductivity remains elusive. They can be simply coexisting, competing or even intertwined with superconductivity, and their impact on the superconducting transition temperature is often unclear. Understanding the normal state of unconventional superconductors is generally the first important step towards unveiling the mechanism of superconductivity in these materials.
In this thesis, we study the superconductor BaNi2As2 which is structurally identical to the parent compounds of high-temperature Fe-based superconductors, BaFe2As2, but exhibits a completely different set of electronic phases, none of them being in particular magnetic in nature. Recently, investigations of Sr substituted Ba1-xSrxNi2As2 attracted attention with a sixfold enhancement of Tc and the discovery of an electronic nematic phase by elasto-resistance measurements [1]. Here, we have explored the effect of an alternative substitution. In this talk, I present the first study of novel Ca-substituted Ba1-xCaxNi2As2. First, we report the growth procedure for the synthesis of high-quality single crystals with a substitution level of up to 10 %. The main goal is to create a first phase diagram for Ba1-xCaxNi2As2 based on specific heat and electrical transport measurements. In this context, we determined the temperatures of a triclinic transition TS, a minimum in dR/dT Tmin, and the superconducting transition Tc for several samples. We observed a decrease of TS from 137 K to below 100 K (on cooling) and a slow increase of Tc by about 0.2 K, an observation which strongly contrasts to that made upon Sr substitution in the absence of a significant contraction of the unit cell. In addition, we have carried out a first study of the lattice dynamics of this system, focusing in particular on the behavior of the Eg,1 Raman active vibration. Earlier studies had revealed a new type of lattice-driven nematicity [2] and its occurrence in the Ca-substituted system was studied.
[1] Eckberg et al., Nature Physics 16, 346-350 (2020)
[2] Yao et al., (2022)

Mi 14:00
Online - Zoom Meeting
Santanu Pakhira
Ames Laboratory
Novel magnetism in 122-type itinerant pnictide system and Eu-based magnetic topological materials

The 122-type iron pnictides have opened up a wide research field after the discovery of superconductivity (SC) with chemical doping by suppressing the long-range antiferromagnetic (AFM) order of parent compounds. In the absence of SC, isotructural cobalt pnictides are itinerant quantum magnets and are described to consist of competing magnetic interactions. In the first part of my talk, I will present the novel magnetic properties of some doped ACo2As2 (A = Ca, Sr) compounds. CaCo2-yAs2 is a unique itinerant magnetic system with strong frustration and exhibits A-type antiferromagnetic (AFM) ordering below TN ≈ 52 K. Although frustration in local moment systems are well studied, itinerant frustrated magnetic systems are largely unexplored. Such magnetically unstable states are fragile and can be easily chemically tuned to different exotic quantum states. Both electron- and hole-doping onto the Co-site through Fe and Ni substitutions strongly suppress the AFM ordering in the system followed by a carrier-tuned Stoner transition [1, 2]. In the absence of long-range magnetic ordering, strong quasi-1D ferromagnetic quantum spin-fluctuations develop in these doped-CaCo2-yAs2 along with a signature of non-Fermi-liquid behavior. In SrCo2As2, no long-range magnetic order is detected in down to at least 50 mK, but stripe AF spin fluctuations exist. We found that Pd substitution trigger long-range AF order in the system. In the second part of my talk I will discuss some of the important results on Eu-based magnetic topological materials. Understanding the complex interplay of magnetism and band topology is quite important to discover exotic quantum phenomena in magnetic topological materials. Recently, topological Dirac surface states are reported in trigonal A-type AFM compounds EuMg2Bi2 and EuSn2As2. We have shown that in the AFM state, an unusual low-field induced spin reorientation in the three-fold AFM domains is observed for both the compounds associated with a weak in-plane anisotropy. H-T magnetic phase diagrams are constructed from the combined results of magnetic, heat capacity, resistivity, and neutron diffraction data [3, 4]. The phase boundary between the AFM and PM states is consistent with the molecular-field-theory prediction for spin S = 7/2.
[1] B. G. Ueland et. al., Phys. Rev. B 104 (2021) L220410
[2] S. Pakhira et. al., Phys. Rev. B 104 (2021) 094420
[3] S. Pakhira et. al., Phys. Rev. B 101 (2020) 214407
[4] S. Pakhira et. al., Phys. Rev. B 104 (2021) 174427

Mi 11:00
Hybrid Zoom / CN B.425 R.206
Mads Hansen
Institut Néel, CNRS
LaFeSiO1-δ: A Novel Superconducting Member of the Iron-Silicide Family

Since their discovery in 2008, iron-based superconducting pnictides (As, P...) and chalcogenides (Te, Se...) have become a well-established class of unconventional superconductors, spanning multiple structural families, with Tc up to 55 K in bulk materials [1]. This category of superconductors has recently been extended to a new subgroup of materials where pnictogen/chalcogen atoms are replaced by Si in LaFeSiH (Tc ~ 10 K) and LaFeSiFx (Tc ~ 9 K) [2,3].
By using a topotactical approach, we were able to intercalate oxygen in intermetallic LaFeSi, resulting in the novel crystallogenide, LaFeSiO1-δ. Our study, based on complementary experimental probes, reveals that this crystallogenide is superconducting with Tc ~ 10 K [4].
Considering its strongly squeezed Fe-Si anion height, below 1 Å, this Tc is surprisingly high, challenging the quasi-universal relationship between structure and superconductivity in Fe-based compounds [5]. The unique crystal structure of this new compound has a strong impact on its electronic properties where the doping is absorbed in a non-rigid-band fashion, resulting in a distinct fermiology. Specifically, the electron pockets, usually observed around the M point in the prototypical Fermi surface of iron-based superconductors, are strongly suppressed, while the hole-like pockets at the Γ point are retained. This, in turn, is detrimental to the usual (π,π)-nesting. The lack of such nesting suggests a departure from s± pairing mechanism.
Furthermore, above Tc, resistivity shows a non-Fermi liquid behaviour, implying significant electronic correlations. This correlated behaviour is also visible in NMR where anti-ferromagnetic fluctuations are observed at low temperatures.
[1] H. Hosono, K. Kuroki, Physica C 514, 399 (2015).
[2] F. Bernardini et al., Phys. Rev. B 97, 1462 (2018).
[3] J.-B. Vaney et al., Nature Communications. 13, 100504 (2022).
[4] M. F. Hansen et al., npj Quantum Materials - in review (2021).
[5] C. H. Lee et al, Solid State Communications, 152, 8 (2012)

Di 16:00
Hybrid Zoom / CS Sem.R. 3.01
Philippe Goldner
Chimie Paristech, ENS Paris
Emerging Rare Earth-Based Platforms for Optical Quantum Technology

Mi 11:00
Hybrid Zoom / CN B.425 R.206
Jazmín Aragón Sanchez
Centro Atómico Bariloche, CNEA, CONICET Universidad Nacional de Cuyo, Argentina
Impact of atomic defects in the bulk electronic states of FeSe1-xSx superconducting crystals

Understanding the impact of atomic-scale defects in the electronic structure of Fe-based superconductors is of key importance for assessing how critical are the occurrence of these features for the establishment of superconductivity in these compounds. With this aim, here we study single crystals of FeSe1-xSx, the Fe-based compound with the simplest crystal structure, consisting of a pile up of superconducting layers. We apply scanning tunnelling microscopy (STM) to reveal that this compound presents S-doping induced defects as well as diluted dumbbell defects associated to an Fe vacancy. We measure the electronic structure of the samples by means of X-ray photoemission spectroscopy (XPS) and reveal that the spectral shape of the peaks of some of the Se and Fe core levels can only be adequately described by considering a dominant plus a smaller second component of the electronic states. We find this result for both, pure as well as S-doped samples, irrespective that they present extra crystal defects associated to the substitution of Se by S atoms. Structural and resistivity characterization, as well as the spectral shape and energy location of the peaks in XPS spectra, indicate our samples do not present intergrowths of the hexagonal phase. Even though in our STM topographies only about 4% of the imaged Se atoms are involved in dumbbell defects, according to DFT calculations these defects entail a significant modification of the electronic clouds of the eight Se and Fe atoms surrounding the Fe vacancy. Furthermore, in the case of FeSe films, if the density of dumbbells increases, superconductivity is suppressed. Thus, we suggest the second component in our XPS spectra is associated to the ubiquitous dumbbell defects in FeSe. These impact of atomic defects in the binding energy energy and spectral shape of the core levels in FeSe1-xSx highlights the subtle interplay between the crystal structure and the bulk electronic states in Fe-based superconductors.

Di 16:00
Hybrid Zoom / CS Sem.R. 3.01
Yanina Fasano
Centro Atómico Bariloche, CNEA, CONICET, Universidad Nacional de Cuyo, Argentina
Leibniz Institute for Solid State and Materials Research, Dresden
Hyperuniformity in Vortex Matter in type-II Superconductors

Many biological, material and mathematical systems share the special property of being hyperuniform, namely of presenting vanishing infinite-wavelength density fluctuations. This means that the density of the constituent objects is homogeneous in the large scale, as in a perfect crystal, although they can be isotropic and disordered like a liquid. Hyperuniform structures present a structure factor that algebraically decays to zero when decreasing the reciprocal-space wavenumber q due to the suppression of particle density fluctuations at large direct-space length-scales. This "hidden order" present in disordered systems can be affected by the type of disorder of the host medium where the objects are nucleated. Vortex matter nucleated at the surface of superconducting samples with weak point-like disorder are ordered and disordered hyperuniform systems.[1,2] In this work we study experimentally and theoretically how planar correlated disorder in the medium affects this property. We show that correlated strong disorder generated by planes of defects traversing the whole sample thickness suppress the hyperuniformity of the structure. This particular type of disorder produces a structure factor that decays at small wavenumbers but saturates in the limit q->0 due to persisting vortex density fluctuations at large lengthscales. We also show that this suppression is concomitant to anisotropic vortex density fluctuations.
[1] G. Rumi, J. Aragón Sánchez, F. Elías, R. Cortés Maldonado, J. R. Puig, N. R. Cejas Bolecek, G. Nieva, M. Konczykowski, Y. Fasano, A.B. Kolton, Phys. Rev. Res. 1 (2019) 033057
[2] J. B. Llorens, I. Guillamón, I. García-Serrano, R. Córdoba, J. Sesé, J.M. De Teresa, M. R. Ibarra, S. Vieira, M. Ortuño, H. Suderow, Phys. Rev. Res. 2 (2020) 033133

Mi 16:00
Join Zoom Meeting
Susmita Roy
University of Colorado, Boulder
Conventional, Time-Resolved Raman, and Inelastic Neutron Scattering of Strongly Correlated Materials

The interplay between charge, spin and lattice degrees of freedom creates exotic phases in strongly correlated materials. Raman and Neutron scatterings are valuable tools to study these phases because of their sensitivity towards these elementary excitations. I will first present the time-resolved Raman scattering results on optimally doped YBa2Cu3O6.9 superconductor which focuses on relaxation timescales and interactions between electrons and phonons. Experimental advances we have made allow for future time-resolved experiments in which the pump frequency can be tuned from the near-to mid-infrared, opening the possibility to pump particular infrared-active modes and observe their effect on Raman-active modes. Further, I will discuss the Raman scattering results which will illuminate the impact of flash sintering on the structure of layered oxide structure of cuprate Pr2CuO4. The combined comprehensive inelastic neutron scattering measurements of Ba8Ga16Ge30 with lattice dynamical calculations based on the density functional theory will be presented to elucidate the effect of the occupational disorder on heat-carrying phonons. Also, I will show the Raman scattering results of spin- 1/2 quantum spin liquid Ba4Ir3O10 which will provide the signatures of spinons and damped phonons.

Di 16:00
IQMT & PHI Seminar / Hybrid Zoom & CS-P R. 3-1
Yolita Eggeler
Laboratorium für Elektronenmikroskopie des Karlsruher Instituts für Technologie
Exploring Magnetic Phenomena on the Nanoscale of Functional Materials Using Analytical In Situ Transmission Electron Microscopy

Mi 11:00
Hybrid Zoom / CN B.425 R.206
Huanhuan Shi
TU Dresden
Exfoliation and Functionalization of 2D Semiconductors via Wet Chemistry

2D semiconductors have remarkable physical, optical and electrical properties and high surface areas. These intrinsic properties make 2D semiconductors promising candidates for versatile applications such as (opto)electronics, energy storage and conversion. However, scalable synthesis of high quality 2D semiconductors remains a significant barrier for their device integrations and practical applications. Therefore, the development of a novel chemical exfoliation process which aims at high yield synthesis of high quality 2D materials while maintaining good solution processability is of great concern.
Here, we focus on the solution production of emerging 2D materials (In2Se3 , MXene and black phosphorus) with high-quality by wet-chemical exfoliation methods and address their applications for high performance (opto)electronics and supercapacitors.
[1] H. Shi, M. Li, A. Shaygan Nia, M. Wang, S. Park, Z. Zhang, M. R. Lohe, S. Yang, X. Feng, Adv. Mater. 32 (2020) 1907244
[2] H. Shi, P. Zhang, Z. Liu, S. Park, M. R. Lohe, Y. Wu, A. S. Nia, S. Yang, X. Feng, Angew. Chem., Int. Ed. 60 (2021) 8689
[3] H. Shi, S. Fu, Y. Liu, C. Neumann, M. Wang, H. Dong, P. Kot, M. Bonn, H. Wang, A. Turchanin, Oliver G. Schmidt, A. Shaygan Nia, S. Yang, X. Feng, Adv. Mater. 33 (2021) 2105694

Fr 11:00
Hybrid Zoom / CN B.425 R.206
Alexander Grimm
Quantum Information Processing with Schrödinger-Cat Qubits

Quantum two-level systems are routinely used to encode qubits but tend to be inherently fragile, leading to errors in the encoded information. Quantum error correction (QEC) addresses this challenge by encoding effective qubits into more complex quantum systems. Unfortunately, the hardware overhead associated with QEC can quickly become very large.
In contrast, a qubit that is intrinsically protected against a subset of quantum errors can be encoded into superpositions of two opposite-phase oscillations in a resonator, so-called Schrödinger-cat states. This "Schrödinger-cat qubit" has the potential to significantly reduce the complexity of QEC. In a recent experiment, we have demonstrated the stabilization and operation of such a qubit through the interplay between Kerr nonlinearity and single-mode squeezing in a superconducting microwave resonator.
In this talk, I will review some key concepts of QEC and situate our approach within the field. I will give an overview of the cat qubit, followed by an outlook on different applied and fundamental research directions it enables.

Fr 14:00
Zoom Seminar
Wahib Aggoune
Institut für Physik & IRIS Adlershof Humboldt-Universität zu Berlin
Tuning two-dimensional electron and hole gases at LaInO3/BaSnO3 interfaces by polar distortions, termination, and thickness

Two-dimensional electron gases (2DEG), arising due to quantum confinement at interfaces between transparent conducting oxides, have received tremendous attention in view of electronic applications. The challenge is to find a material system that exhibits both a high charge-carrier density and mobility at room temperature. In this talk, we will explore the potential of interfaces formed by two lattice-matched wide-gap oxides of emerging interest, i.e., the polar, orthorhombic perovskite LaInO3 and the non-polar, cubic perovskite BaSnO3, employing density-functional theory and many-body perturbation theory. We first present the properties of the pristine components. For periodic heterostructures, we show that the polar discontinuity at the interface is mainly compensated by electronic relaxation through charge transfer from the LaInO3 to the BaSnO3 side. This leads to the formation of a 2DEG hosted by the highly-dispersive Sn-s-derived conduction band and a 2D hole gas of O-p character, strongly localized inside LaInO3. Remarkably, structural distortions through octahedra tilts induce a depolarization field counteracting the polar discontinuity, and thus increasing the critical (minimal) LaInO3 thickness, required for the formation of a 2DEG. These polar distortions decrease with increasing LaInO3 thickness, enhancing the polar discontinuity and leading to a 2DEG density f 0.5 electron per unit-cell surface. Interestingly, in non-periodic heterostructures, these distortions lead to a decrease of the critical thickness, thereby enhancing and delocalizing the 2DEG. We rationalize how polar distortions, termination, and thickness can be exploited in view of tailoring the 2DEG characteristics, and why this material is superior to the most studied prototype LaAlO3/SrTiO3.

Di 16:00
Zoom Seminar
Xing He
Mechanical Engineering and Materials Science, Duke University, Durham, North Carolina, USA
Understanding Phonon Anharmonicity Using Neutron / X-ray Scattering and First-Principles Simulation

Phonon anharmonicity is crucial to understand thermal transport properties of materials, phase transition mechanisms, as well as atomic disorder/diffusions. Time-of-flight inelastic neutron scattering instrument covering large four-dimensional momentum and energy space, is suitable to probe phonon frequencies and lifetimes as a function of temperature. Moreover, first-principles simulation including temperature effects, such as ab initio molecular dynamics, and recent machine-learning accelerated molecular dynamics provide tools for large atomic scale and time scale analysis of anharmonic systems. In this talk, we combine inelastic neutron scattering, neutron/x-ray diffuse scattering, and first-principles calculation to probe and decipher phonon anharmonicities in multiple perovskite materials for both oxide and halide. Oxide perovskites, exhibiting multiple phase transitions and lattice instability and complex ferroelectric polarization behaviors, have drawn interest for decades, with recent emerging quantum critical behaviors, anomalous thermal transport properties, and thermal hall effects at low temperature. While halide perovskite, softer than oxide, has attracted attention due to high performance in photovoltaic, radiation detectors, potential thermoelectric materials, and optoelectronic properties coupling with large atomic fluctuation. Here, we probe and rationalize the phonon eigenvector anharmonicity in oxide perovskite as approaching quantum critical point, large octahedron instability and strong diffuse scattering in halide perovskite, and selective coupling of atomic disorder with phonons in oxide perovskite.
[1] Xing He et al., Phys. Rev. Lett. 124 (2020) 145901
[2] T. Lanigan-Atkins, Xing He et al., Nat. Mater. 20 (2021) 977
[3] Xing He et al., arXiv preprint arXiv:2112.04717 (2021)

Di 16:00
Zoom Seminar
Senthil Kumar Kuppusamy
Coherent light-matter interactions in rare-earth ion containing molecules

Di 16:00
Zoom Seminar
Evgeni Ilichev
Leibniz Institute of Photonic Technology, Jena
Dual Shapiro Steps in Superconducting Nanowire

We demonstrated current quantization in a superconducting NbN nanowire subject to microwave radiation. The observed current steps, dual to Shapiro steps in Josephson junctions, result from photon assisted tunneling of coherent quantum phase slips. To suppress fluctuations the nanowires are incorporated into a compact high impedance environment. Without radiation the nanowires exhibit supercurrent-like behavior at high bias and current blockade at low bias. The demonstrated effect is promising for the development of the quantum current standard; a missing element in the Quantum Metrology Triangle. We observe the effect with radiation up to 31 GHz, and sharp steps up to 26 GHz, corresponding to a current step of 8.3 nA.

Di 16:00
Zoom Seminar
Patrick Winkel
Superconducting Quantum Circuits for Hybrid Architectures

Superconducting quantum circuits (SQCs) constitute a versatile hardware platform for the realization of novel quantum technologies. While the quantum coherence of SQCs has been improved significantly over the last two decades, there are other quantum degrees of freedom, which outperform SQCs in some figures of merit. For that reason, it might proof beneficial to combine these different technologies in a quantum hybrid architecture. Within the scope of my PhD thesis, I developed a non-linear inductive circuit element based on granular aluminum (grAl) - a disordered superconductor with high kinetic inductance - which can be operated in strong external magnetic fields, an essential requirement for the applicability in a hybrid system. As a proof of concept, the quantum coherence and non-linearity of the element is demonstrated by the implementation of a transmon qubit, in which the conventional Josephson junction is substituted by the grAl element. In order to improve the signal-to-noise ratio of the measurement, I developed a non-degenerate parametric amplifier based on long arrays of Josephson junctions, with up to 1800 elements. The novelty of the amplifier concept is to use multiple eigenmodes to cover the desired frequency range between 1 and 10 GHz.