JWJoachim Wosnitza

Joachim Wosnitza

*This is an algorithmically generated author record based on publicly available information.

Current Organizations / Institutes

The organizations/institutes from the scholar's latest article

Previous Organizations / Institutes

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Joachim Wosnitza has a total of 110 co-authors. Here are the top co-authors by number of shared publications:


Latest Publications

  • Elastic Softening in Synthetic Diamonds

    by Tatsuya Yanagisawa, Ruo Hibino, Hiroyuki Hidaka, Hiroshi Amitsuka, Toshiyuki Tashima, Mitsuhiro Akatsu, Yuichi Nemoto, Sergei Zherlitsyn, Joachim Wosnitza

  • Multicalorics II

    by J. Wosnitza, J. Slaughter, Q. M. Zhang, H. Hou

  • Open Access

    Gate-controlled superconductivity and quantum interference in 300 mm CMOS-compatible ZrN nanostructures

    by Roman Potjan, Oliver Ostien, Marcus Wislicenus, Raik Hoffmann, Katharina Lilienthal, Kilian Heidner, Felix Mende, Sergej Liberda, André Reck, Varvara Brackmann, et al.

    The interplay of alternative materials, large-scale integration technologies, and innovative devices plays a pivotal role on the way to fault-tolerant quantum computing. In this context, gate-controlled superconductivity (GCS) emerges as a key enabling technology, promising to advance superconducting logic and quantum electronics, complementing conventional approaches based on Josephson effects and quantum interference. Here, we demonstrate all-metallic superconducting ZrN nanostructures on silicon, fabricated entirely using a subtractive, monolithic dry-etch approach with a 300 mm CMOS-compatible process flow. For Dayem-bridge weak links with decreasing width down to 27 nm, we observe Tc of 7.3 K, width-dependent switching characteristics, and a progressive approach of the tunneling limit. In laterally gated Dayem-bridge and nanowire devices, we observe GCS with full suppression of the critical current, where required gate voltages <5 V promise compatibility with CMOS interfaces. Asymmetries in polarity-dependent power injection via field emission support GCS models that attribute the effect to quasiparticle relaxation through phonon emission. Additional asymmetries in the GCS effect suggest an influence of the substrate condition after dry etching. Field emission features in the gated nanowire device imply superimposed current paths along the gate edge and corners. Finally, we analyze magnetic interference in Dayem-bridge weak links and superconducting quantum interference devices, where quantum interference is governed by Josephson effects and inductance loop asymmetries. Our results contribute to the scaling efforts in hybrid superconducting electronics and quantum-processing units.


  • Open Access

    Magnetocaloric effect in La1−zCez(Fe0.88−yMnySi0.12)13 with tunable, low transition temperature in high magnetic fields

    by M. Straßheim, C. Salazar Mejía, E. Bykov, T. Niehoff, L. Beyer, J. Freudenberger, R. Hübner, F. Ganss, T. Naumann, J. Wosnitza, et al.

    Cryogenic magnetic refrigeration becomes more and more important nowadays, especially for the liquefaction of gases such as hydrogen. In this study, we have synthesized La1−zCez(Fe0.88−yMnySi0.12)13 samples and investigated their magnetic and magnetocaloric properties in order to assess their potential for cryogenic applications. By adjusting the Mn and Ce content and adding excess rare-earth elements, the first-order ferromagnetic transition was lowered from 200 to 40 K and the adiabatic temperature change of the samples was measured directly using pulsed magnetic fields. The sample with the lowest transition temperature still showed a significant adiabatic temperature change in magnetic fields up to 10 T, with an increasingly stronger first-order transition observed in samples with higher Ce substitution. In addition, we synthesized spherical powder with diameters between 20 and 120 μm using ultrasonic atomization while maintaining the magnetic transition, which is a promising starting material for future additive manufacturing of magnetocaloric materials.


  • Open Access

    300 mm CMOS-compatible superconducting HfN and ZrN thin films for quantum applications

    by Roman Potjan, Marcus Wislicenus, Oliver Ostien, Raik Hoffmann, Maximilian Lederer, André Reck, Jennifer Emara, Lisa Roy, Benjamin Lilienthal-Uhlig, J. Wosnitza

    The rising interest in increased manufacturing maturity of quantum processing units is pushing the development of alternative superconducting materials for semiconductor fab process technology. However, these are often facing CMOS process incompatibility. In contrast to common CMOS materials, such as Al, TiN, and TaN, reports on the superconductivity of other suitable transition-metal nitrides are scarce, despite potential superiority. Here, we demonstrate fully CMOS-compatible fabrication of HfN and ZrN thin films on state-of-the-art 300 mm semiconductor process equipment, utilizing reactive DC magnetron sputtering on silicon wafers. Measurement of mechanical stress and surface roughness of the thin films demonstrates process compatibility. We investigated the materials phase and stoichiometry by structural analysis. The HfN and ZrN samples exhibit superconducting phase transitions with critical temperatures up to 5.84 and 7.32 K, critical fields of 1.73 and 6.40 T, and coherence lengths of 14 and 7 nm, respectively. A decrease in the critical temperature with decreasing film thickness indicates mesoscopic behavior due to geometric and grain-size limitations. The results promise a scalable application of HfN and ZrN in quantum computing and related fields.


  • Open Access

    Huge magnetostriction in superconducting single-crystalline BaFe1.908Ni0.092As2

    by Minjie Zhang, Jiating Wu, Ke Shi, Langsheng Ling, Wei Tong, Chuanying Xi, Li Pi, J. Wosnitza, Huiqian Luo, Zhaosheng Wang

    The performance of iron-based superconductors in high magnetic fields plays an important role for their practical application. In this work, we measured the magnetostriction and magnetization of BaFe1.908Ni0.092As2 single crystals using pulsed magnetic fields up to 60 T and static magnetic fields up to 33 T, respectively. A huge longitudinal magnetostriction (of the order of 10–4) was observed in the direction of twin boundaries. The magnetization measurements evidence a high critical-current density due to strong bulk pinning. By using magnetization data with an exponential flux-pinning model, we can reproduce the magnetostriction curves qualitatively. This result shows that the magnetostriction of BaFe1.908Ni0.092As2 can be well explained by a flux-pinning-induced mechanism.


  • Open Access

    Highly sensitive band structure of the Stoner-enhanced Pauli paramagnet SrCo2P2

    by K. Götze, I. Kraft, J. Klotz, T. Förster, M. Uhlarz, V. Lorenz, C. Bergmann, Y. Prots, J. A. N. Bruin, A. McCollam, et al.

    The compound SrCo2P2 is a Pauli paramagnet very close to ferromagnetic order. To study its electronic structure in close vicinity to the Fermi level, we report measurements of the de Haas–van Alphen effect in magnetic fields up to 35 T in combination with density-functional-theory band-structure calculations in different approximations. The resulting electronic band structure not only depends significantly on the choice of the functional, but also crucially on the exact values of the structural parameters that have been determined at low temperatures by synchrotron x-ray diffraction. We find the best correspondence between the measured and the calculated de Haas–van Alphen frequencies for the general gradient approximation functional and the structural parameters that were determined at 10 K. Although SrCo2P2 crystallizes in the uncollapsed tetragonal structure with a large P-P distance between the Co2P2 layers, we observe a rather three-dimensional Fermi-surface topology. We obtain a mass-enhancement factor of about 2 deduced from the ratio between experimental and calculated quasiparticle masses. The temperature dependence of the structural parameters leads to a significant reduction of the electronic density of states at the Fermi level and in comparison with the measured Sommerfeld coefficient to an overall mass renormalization in line with our experiment.


  • Open Access

    Magnetic excitations in the spin-1/2 triangular-lattice antiferromagnet Cs2CuBr4

    by S A Zvyagin, M Ozerov, D Kamenskyi, J Wosnitza, J Krzystek, D Yoshizawa, M Hagiwara, Rongwei Hu, Hyejin Ryu, C Petrovic, et al.


  • Open Access

    Fermi surface of the superconductorBaIr2P2

    by T. Förster, B. Bergk, O. Ignatchik, M. Bartkowiak, S. Blackburn, M. Côté, G. Seyfarth, N. Berry, Z. Fisk, I. Sheikin, et al.

    We report on de Haas–van Alphen (dHvA) and band-structure studies of the iridium-pnictide superconductor BaIr2P2 (Tc=2.1 K). The observed dHvA frequencies can be well understood by our band-structure calculations with two bands crossing the Fermi energy leading to a strongly corrugated Fermi-surface cylinder around the X point and a highly evolved, multiconnected Fermi surface extending over the whole Brillouin zone. The experimental effective masses are found to be considerably larger than the calculated band masses suggesting strong many-body interactions. Nevertheless, Tc remains only moderate in BaIr2P2 contrary to isostructural iron pnictides which probably is related to the largely different Fermi-surface topologies in these materials.


  • Open Access

    Fermi-surface topology of the iron pnictideLaFe2P2

    by S. Blackburn, B. Prévost, M. Bartkowiak, O. Ignatchik, A. Polyakov, T. Förster, M. Côté, G. Seyfarth, C. Capan, Z. Fisk, et al.

    We report on a comprehensive de Haas–van Alphen (dHvA) study of the iron pnictide LaFe2 P2. Our extensive density-functional band-structure calculations can well explain the measured angular-dependent dHvA frequencies. As salient feature, we observe only one quasi-two-dimensional Fermi-surface sheet; i.e., a hole-like Fermi-surface cylinder around Γ, essential for s± pairing, is missing. In spite of considerable mass enhancements due to many-body effects, LaFe2 P2 shows no superconductivity. This is likely caused by the absence of any nesting between electron and hole bands.