@book{62182,
  abstract     = {{<p> Executive summary Die vorliegende Zukunftsstudie „Automation 2035“ gibt einen Ausblick auf die Entwicklung der Automatisierungstechnik in den nächsten 10 Jahren. Neben der Beschreibung von Trends wie Kreislaufwirtschaft, Automatisierung der Märkte, Biologisierung, autonome Systeme und Robotik sowie IT-Sicherheit wird die zu erwartende Veränderung in der Bildung beschrieben. Dazu verwenden wir Methoden der Zukunftsforschung und arbeiten mit der Szenarientechnik, um Zukunftsperspektiven der Automation aufzuzeigen. Personas werden eingesetzt, um die zukünftigen Entwicklungen plastisch aus den Augen der Personen im Jahr 2025 und in der Zukunft im Jahr 2035 zu beschreiben. Schlüsselthemen und Trends: ... ... Inhalt Executive summary 1 1 Einführung 3 2 Zukunftsfelder für die Automatisierungstechnik 2035 4 2.1 Kreislaufwirtschaft 4 2.2 Automatisierung der Märkte 7 2.3 Biologisierung 8 2.4 Autonome Systeme und Robotik 10 2.5 Security 12 2.6 Veränderung der Ausbildung 13 3 Szenario der Automation 2035 16 4 Personas 18 4.1 Unternehmer 18 4.2 Ingenieurin 19 4.3 Schüler 20 5 Thesen und Ausblick 22 Methodik 24 Autorenteam 25 Schrifttum 26... </p>}},
  author       = {{Gräßler, Iris and Özcan, Deniz and Tusek, Alena Marie and Bilgic, Attila and Lange, Christian and Stich, Christian and Maul, Christine and Heizmann, Michael and Weyrich, Michael and Dessel,, Sascha and Miny, Torben and Jumar, Ulrich}},
  isbn         = {{9783911670180}},
  publisher    = {{VDI Verlag}},
  title        = {{{Automation 2035}}},
  doi          = {{10.51202/9783911670180}},
  year         = {{2025}},
}

@article{62265,
  author       = {{Schroeter-Wittke, Harald}},
  journal      = {{Praktische Theologie}},
  number       = {{4}},
  pages        = {{254--255}},
  title        = {{{Gott, heilger Schöpfer aller Stern (EG 3). Zum 500. Todestag von Thomas Müntzer (1489-1525)}}},
  volume       = {{60}},
  year         = {{2025}},
}

@inbook{60965,
  author       = {{Bergmann, Claudia Dorit and Latt, May May}},
  booktitle    = {{Imitating Abraham: Ritual and Exemplarity in Jewish and Christian Contexts}},
  editor       = {{Bergmann, Claudia D. and Blanton, Thomas R.}},
  pages        = {{35--58}},
  publisher    = {{Brill}},
  title        = {{{'Look to Abraham and Sarah'}}},
  year         = {{2025}},
}

@phdthesis{62748,
  abstract     = {{Erklärungen spielen eine zentrale Rolle in alltäglichen persönlichen Gesprächen, indem sie den Wissensaustausch fördern, Ideen klären und das Verständnis unterstützen. In solchen Gesprächen versuchen die Erklärenden (d. h. die sachkundigere Person), das Verständnis der Explainees (d. h. die Person, die eine Erklärung erhält) durch Interaktionsprozesse wie Monitoring, Scaffolding und gemeinsame Konstruktion zu verbessern (Buschmeier et al., 2023; Rohlfing et al., 2021). Während gemeinsame Konstruktionen aus dem bidirektionalen (non-)verbalen Austausch zwischen den Gesprächspartnern entstehen, bezeichnet Scaffolding den Prozess, durch den die Erklärenden eine Erklärung anpassen, indem sie unterschiedliche Verhaltensweisen als Reaktion auf das Verhalten der Explainees einsetzen, welches deren kognitive Verarbeitung signalisiert (Wood et al., 1976). Monitoring bezeichnet einen kontinuierlichen Prozess, in dem die Gesprächspartner auf Wahrnehmungssignale wie (non-)verbale Verhaltensweisen achten, um Hinweise auf (Miss-)Verständnisse zu erkennen und zu interpretieren (Clark &amp; Krych, 2004).In der vorliegenden Arbeit berichte ich über fünf Studien zu dyadischen Erklärungen zwischen Menschen und diskutiere anhand empirischer Befunde die Interaktionsdynamiken, die bestimmten Formen verbalen und nonverbalen Erklärungsverhaltens zugrunde liegen. Zu diesem Zweck analysierte ich in den vorgestellten Studien Daten aus zwei Videokorpora zu verschiedenen Bereichen alltäglicher Erklärungen, beispielsweise medizinischen Erklärungen und Brettspielerklärungen. Das Korpus zu medizinischen Erklärungen umfasst elf naturalistische Interaktionen zwischen Ärzten und Bezugspersonen über eine bevorstehende chirurgische Operation von Kindern. Das Korpus zu Brettspielerklärungen besteht aus 87 dyadischen Brettspielerklärungen, von denen eine Teilstichprobe von 24 Interaktionen in den vorgestellten Studien spezifisch untersucht wurde.Um das verbale Erklärungsverhalten zu untersuchen, analysierte ich in zwei Studien, die sich mit medizinischen Erklärungen und Brettspielerklärungen befassten, den Zusammenhang zwischen Themenwechseln in Erklärungen und dem multimodalen Verhalten der Explainees, das von den Erklärenden beobachtet wurde. Die Analyse medizinischer Erklärungen legt nahe, dass der Wechsel von Elaborationen zu neuen Themen mit dem multimodalen Verhalten der Explainees einhergeht, welches Blickabwendung, Kopfnicken und verbale Rückkopplung umfasst. Der Wechsel zu Elaborationen hingegen ist mit einer anhaltenden Blickrichtung verbunden, unabhängig davon, ob zusätzliche Signale vorhanden sind oder nicht (Lazarov et al., 2024). Eine nachfolgende Studie zu Brettspielerklärungen (Lazarov &amp; Grimminger, in Begutachtung) erweiterte diese Analyse durch die Einbeziehung des Blickverhaltens der Erklärenden. Die Studie untersuchte den Zusammenhang zwischen gegenseitigem Blickkontakt und Blickabwendung mit der Einleitung neuer Themen. Die Ergebnisse bestätigten die Ergebnisse aus dem medizinischen Kontext: Blickabwendungen der Explainees gehen Themenwechseln häufiger voraus als gegenseitiger Blickkontakt, was mit früheren Forschungsergebnissen von Rossano (2012, 2013) übereinstimmt. Die Analyse untersuchte zudem den Zusammenhang zwischen dem / der Gesprächspartner:in, der / die Blickabwendungen initiierte, und dem / der Gesprächspartner:in, der / die Themenwechsel initiierte.Um das nonverbale Erklärungsverhalten zu untersuchen, analysierte ich die Verwendung von sprachbegleitenden Gesten von verschiedenen Erklärenden in drei Studien zu Brettspielerklärungen, in denen das zu erklärende Objekt im gemeinsamen Referenzraum physisch nicht vorhanden war. Obwohl diese Abwesenheit ein fortwährendes Bedürfnis nach der Etablierung gemeinsamer imaginärer Räume impliziert (Kang et al., 2015; Kinalzik &amp; Heller, 2021), beispielsweise durch kontinuierliches Zeigen auf unsichtbare Orte, zeigte die Studie von Lazarov &amp; Grimminger (2025), dass Gestenikonizität und zeitliche Hervorhebung auch in Themen zu Objekteigenschaften, Handlungsprozessen und bedingten Regeln variabel auftreten.Motiviert durch die kontinuierliche Verwendung von der gestischen Deixis während der physischen Abwesenheit des Explanandums erforschten die letzten zwei Studien den kognitiven Mechanismus der Anpassung des Gebrauchs deiktischer Gesten in Bezug auf die Beobachtung des Verständnisses der Explainees. Unabhängig davon, ob die Erklärenden das Verständnis der Explainees in einer retrospektiven Video Recall Aufgabe interpretierten (Lazarov &amp; Grimminger, 2024a) oder die verbalen Verständnissignale der Explainees wahrnahmen (Lazarov &amp; Grimminger, 2024b), zeigten die Analysen, dass die Häufigkeit der gestischen Deixis während der Erklärungsphase, in der das Explanandum nicht im gemeinsamen Raum vorhanden war, stabil blieb. Zu den Ergebnissen der in dieser Dissertation präsentierten Studien diskutiere ich, wie die kontinuierliche Beobachtung des Feedbackverhaltens der Explainees Anpassungen sowohl im verbalen als auch im nonverbalen Erklärungsverhalten erläutern kann. Darüber hinaus verdeutlichen die von mir präsentierten Studien das Ausmaß der individuellen Variation innerhalb und zwischen den Erklärenden, von denen jeder / jede mit drei verschiedenen Explainees interagierte.}},
  author       = {{Lazarov, Stefan Teodorov}},
  pages        = {{167}},
  publisher    = {{Universitätsbibliothek Paderborn}},
  title        = {{{The reflection of interactional monitoring in the dynamics of verbal and nonverbal forms of explaining}}},
  doi          = {{10.17619/UNIPB/1-2446}},
  year         = {{2025}},
}

@article{62749,
  abstract     = {{Coherent Raman scattering techniques as coherent anti-Stokes Raman scattering (CARS), offer significant advantages in terms of pixel dwell times and speed as compared to spontaneous Raman scattering for investigations of crystalline materials. However, the spectral information in CARS is often hampered by the presence of a nonresonant contribution to the scattering process that shifts and distorts the Raman peaks. In this work, we apply a method to obtain nonresonant background-free spectra based on time-delayed, broadband CARS (TD-BCARS) using an intrapulse excitation scheme. In particular, this method can measure the phononic dephasing times across the full phonon spectrum at once. We test the methodology on amorphous SiO2 (glass), which is used to characterize the setup-specific and material-independent response times, and then apply TD-BCARS to the analysis of single crystals of diamond and ferroelectrics of potassium titanyl phosphate (KTP) and potassium titanyl arsenate (KTA). For diamond, we determine a dephasing time of 𝜏=7.81 ps for the single 𝑠⁢𝑝3 peak.}},
  author       = {{Hempel, F. and Rüsing, Michael and Vernuccio, F. and Spychala, K. J. and Buschbeck, R. and Cerullo, G. and Polli, D. and Eng, L. M.}},
  issn         = {{2469-9950}},
  journal      = {{Physical Review B}},
  number       = {{22}},
  publisher    = {{American Physical Society (APS)}},
  title        = {{{Phonon dephasing times determined with time-delayed broadband coherent anti-Stokes Raman scattering}}},
  doi          = {{10.1103/1ctr-csjy}},
  volume       = {{112}},
  year         = {{2025}},
}

@inproceedings{62754,
  author       = {{Vogelsang, Christoph and Wotschel, Philipp and Janzen, Thomas and Grotegut, Lea}},
  location     = {{Heilbronn}},
  title        = {{{Auf die Prüfung kommt es an! - Handlungsnahe Prüfungsformate in Lehramtsstudiengängen}}},
  year         = {{2025}},
}

@article{62867,
  abstract     = {{<jats:title>ABSTRACT</jats:title>
                  <jats:p>Effective manipulation of photonic spin–orbit coupling (SOC) in microcavities is of fundamental importance within topological photonics and applications. Anisotropic organic single‐crystalline materials can induce abundant SOC phenomenon due to their flexible tunability of molecular geometries, however, the intrinsic relationship between molecular geometries/orientations in 3D space and photonic SOC is lacking. In this study, we design two kinds of 2D organic polymorphs for the construction of organic microcavities to investigate the structure‐performance relationships. In two polymorphic microcavities, two distinctive photonic SOC phenomena are observed regardless of the in‐plane anisotropy of organic polymorphs. Theoretical analysis indicates that the photonic SOC strength is strongly influenced by the synergies between the crystal anisotropy and the tilted collective molecular transition dipole moment. Our results uncover the correlation mechanism between the structure of molecules and photonic SOC and open an avenue to engineer complex photonic SOC by use of organic microstructures towards the development of diverse integrated photonic devices.</jats:p>}},
  author       = {{Ji, Ying and Ma, Xuekai and Huang, Han and Deng, Yibo and Wang, Pingyang and Long, Teng and Li, Yuan and Zhao, Ruiyang and Li, Yunfei and An, Cunbin and Schumacher, Stefan and Gu, Chunling and Liao, Bo and Fu, Hongbing and Liao, Qing}},
  issn         = {{1863-8880}},
  journal      = {{Laser &amp; Photonics Reviews}},
  publisher    = {{Wiley}},
  title        = {{{Molecular Orientation‐Dependent Photonic Spin–Orbit Coupling in Organic Microcavities Filled with 2D Polymorphic Crystals}}},
  doi          = {{10.1002/lpor.202501874}},
  year         = {{2025}},
}

@inproceedings{62882,
  author       = {{Osnabrügge, Malin and Tenberge, Claudia}},
  booktitle    = {{Posterbeitrag im Rahmen der Jahrestagung Digitale Transformation für Schule und Lehrkräftebildung vom 29-30.09.2025 }},
  location     = {{Postdam }},
  title        = {{{Digital-gestützt lehren lernen: Technikbezogenen Unterricht zukunftsfähig gestalten}}},
  year         = {{2025}},
}

@article{62910,
  abstract     = {{<jats:p>Frequency-filtered photon correlations have been proven to be extremely useful in grasping how the detection process alters photon statistics. Harnessing the spectral correlations also permits refinement of the emission and unraveling of previously hidden strong correlations in a plethora of quantum-optical systems under continuous-wave excitation. In this work, we investigate such correlations for time-dependent excitation and develop a methodology to compute efficiently time-integrated correlations, which are at the heart of the photon-counting theory, and subsequently apply it to analyze the photon emission of pulsed systems. By combining this formalism with the —which facilitates frequency-resolved correlations—we demonstrate how spectral filtering enhances single-photon purity and suppresses multiphoton noise in time-bin-encoded quantum states. Specifically, filtering the central spectral peak of a dynamically driven two-level system boosts temporal coherence and improves the fidelity of time-bin entanglement preparation, even under conditions favoring multiphoton emission. These results establish spectral filtering as a critical tool for tailoring photon statistics in pulsed quantum light sources.</jats:p>}},
  author       = {{Bermúdez-Feijóo, Santiago and Zubizarreta Casalengua, Eduardo and Müller, Kai and Jöns, Klaus D.}},
  issn         = {{2643-1564}},
  journal      = {{Physical Review Research}},
  number       = {{3}},
  publisher    = {{American Physical Society (APS)}},
  title        = {{{Spectral correlations of dynamical resonance fluorescence}}},
  doi          = {{10.1103/jmy9-bd3l}},
  volume       = {{7}},
  year         = {{2025}},
}

@article{61982,
  abstract     = {{Doped Co3O4 nanoparticles are investigated via spectro-electrochemistry in the (pre-) oxygen evolution reaction (OER) regime by tracing the absorption signal of the Co3+ d–d transition under applied bias for getting insight into the catalysts activation and the formation of catalytically active phases. In the low potential regime up to 1.37 VRHE, a rise in the optical absorption signal of the [Co3+]oct d–d transition is observed and attributed to a structural change from [Co2+]tet to [Co3+]oct due to an electrochemically induced surface restructuring with water. For applied potentials higher than 1.37 VRHE an overall offset of the absorption spectra in the UV–vis range, equivalent to a darkening of the materials is detected. This is attributed to the formation of a CoOx(OH)y skin layer as supported by high-energy X-ray diffraction (HE-XRD) measurements. We found that the kinetics of the Co3+ states are heavily influenced by the type of dopant with V-doped Co3O4 exhibiting stable Co3+ states (>20 min) while the Mn-doped Co3O4 Co3+ states reduce within 36 s under reductive bias. We conclude that doping Co3O4 with transition metals affects the formation and potential-dependent thickness of the CoOx(OH)y skin layer as the catalytically active phase and the formation of long-time stable surface Co3+ states after activation in the first OER cycle.}},
  author       = {{Kampermann, L. and Klein, J. and Wagner, T. and Kotova, A. and Placke-Yan, C. and Yasar, A. and Jacobse, L. and Lasagna, S. and Leppin, Christian and Schulz, S. and Linnemann, Julia and Bergmann, A. and Roldan Cuenya, B. and Bacher, G.}},
  issn         = {{2155-5435}},
  journal      = {{ACS Catalysis}},
  keywords     = {{electrocatalysis, oxygen evolution reaction, cobalt spinel, operando characterization, spectroelectrochemistry}},
  number       = {{21}},
  pages        = {{18391--18403}},
  publisher    = {{American Chemical Society (ACS)}},
  title        = {{{Operando Analysis of the Pre-OER Activation of Metal-Doped Co<sub>3</sub>O<sub>4</sub> Nanoparticle Catalysts}}},
  doi          = {{10.1021/acscatal.5c03900}},
  volume       = {{15}},
  year         = {{2025}},
}

@article{63223,
  abstract     = {{<jats:title>Abstract</jats:title><jats:p>The quartz crystal microbalance with dissipation monitoring (QCM‐D) is routinely used to investigate structured samples. Here, a simulation technique is described, that predicts the shifts of frequency and half bandwidth, Δ<jats:italic>f<jats:sub>n</jats:sub></jats:italic> and ΔΓ<jats:italic><jats:sub>n</jats:sub></jats:italic>, of a quartz resonator operating on different overtone orders, <jats:italic>n</jats:italic>, induced by structured samples in contact with the resonator surface in liquid. The technique, abbreviated as FreqD‐LBM, solves the Stokes equation in the frequency domain. The solution provides the complex amplitude of the area‐averaged tangential stress at the resonator surface, from which Δ<jats:italic>f<jats:sub>n</jats:sub></jats:italic> and ΔΓ<jats:italic><jats:sub>n</jats:sub></jats:italic> are derived. Because the dynamical variables are complex amplitudes, the viscosity can be complex, as well. The technique naturally covers viscoelasticity. Limitations are linked to the grid resolution and to problems at large viscosity. Validation steps include viscoelastic films, rough surfaces, an oscillating cylinder in a viscous medium, and a free‐floating sphere above the resonator. Application examples are soft adsorbed particles, stiff adsorbed particles, and a large, immobile spherical cap above the resonator, which allows to study the high‐frequency properties of the material in the gap. FreqDLBM runs on an office PC and does not require expert knowledge of numerical techniques. It is accessible to an experimentalist.</jats:p>}},
  author       = {{Johannsmann, Diethelm and Häusner, Paul and Langhoff, Arne and Leppin, Christian and Reviakine, Ilya and Vanoppen, Viktor}},
  issn         = {{2513-0390}},
  journal      = {{Advanced Theory and Simulations}},
  number       = {{7}},
  publisher    = {{Wiley}},
  title        = {{{The Frequency‐Domain Lattice Boltzmann Method (FreqD‐LBM): A Versatile Tool to Predict the QCM Response Induced by Structured Samples}}},
  doi          = {{10.1002/adts.202401373}},
  volume       = {{8}},
  year         = {{2025}},
}

@article{63222,
  abstract     = {{<jats:p>The solid electrolyte interphase (SEI) on the anode of lithium-ion batteries (LIBs) has been studied thoroughly due to its crucial importance to the battery’s long-term performance. At the same time, most studies of the SEI apply ex situ characterization methods, which may introduce artifacts or misinterpretations as they do not investigate the SEI in its unaltered state immersed in liquid battery electrolyte. Thus, in this work, we focus on using the non-destructive combination of electrochemical quartz crystal microbalance with dissipation monitoring (EQCM-D) and impedance spectroscopy (EIS) in the same electrochemical cell. EQCM-D can not only probe the solidified products of the SEI but also allows for the monitoring of viscoelastic layers and viscosity changes of the electrolyte at the interphase during the SEI formation. EIS complements those results by providing electrochemical properties of the formed interphase. Our results highlight substantial differences in the physical and electrochemical properties between the SEI formed on copper and on amorphous carbon and show how formation parameters and the additive vinylene carbonate (VC) influence their growth. The EQCM-D results show consistently that much thicker SEIs are formed on carbon substrates in comparison to copper substrates.</jats:p>}},
  author       = {{Stich, Michael and Leppin, Christian and Krauss, Falk Thorsten and Valdes Landa, Jesus Eduardo and Pantenburg, Isabel and Roling, Bernhard and Bund, Andreas}},
  issn         = {{2313-0105}},
  journal      = {{Batteries}},
  number       = {{7}},
  publisher    = {{MDPI AG}},
  title        = {{{Comparing the SEI Formation on Copper and Amorphous Carbon: A Study with Combined Operando Methods}}},
  doi          = {{10.3390/batteries11070273}},
  volume       = {{11}},
  year         = {{2025}},
}

@article{63224,
  abstract     = {{<jats:p>By monitoring the solidification of droplets of plant latices with a fast quartz crystal microbalance with dissipation monitoring (QCM-D), droplets from Campanula glomerata were found to solidify much faster than droplets from Euphorbia characias and also faster than droplets from all technical latices tested. A similar conclusion was drawn from optical videos, where the plants were injured and the milky fluid was stretched (sometimes forming fibers) after the cut. Rapid solidification cannot be explained with physical drying because physical drying is transport-limited and therefore is inherently slow. It can, however, be explained with coagulation being triggered by a sudden decrease in hydrostatic pressure. A mechanism based on a pressure drop is corroborated by optical videos of both plants being injured under water. While the liquid exuded by E. characias keeps streaming away, the liquid exuded by C. glomerata quickly forms a plug even under water. Presumably, the pressure drop causes an influx of serum into the laticifers. The serum, in turn, triggers a transition from a liquid–liquid phase separated state (an LLPS state) of a resin and hardener to a single-phase state. QCM measurements, optical videos, and cryo-SEM images suggest that LLPS plays a role in the solidification of C. glomerata.</jats:p>}},
  author       = {{Langhoff, Arne and Peschel, Astrid and Leppin, Christian and Kruppert, Sebastian and Speck, Thomas and Johannsmann, Diethelm}},
  issn         = {{2223-7747}},
  journal      = {{Plants}},
  number       = {{5}},
  publisher    = {{MDPI AG}},
  title        = {{{Rapid Solidification of Plant Latices from Campanula glomerata Driven by a Sudden Decrease in Hydrostatic Pressure}}},
  doi          = {{10.3390/plants14050798}},
  volume       = {{14}},
  year         = {{2025}},
}

@article{63226,
  abstract     = {{<jats:p>Nanobubbles in water splitting are recognized by the EQCM-D. They are ubiquitous. Lifetimes are in the range of seconds.</jats:p>}},
  author       = {{Leppin, Christian and Langhoff, Arne and Johannsmann, Diethelm}},
  issn         = {{1463-9076}},
  journal      = {{Physical Chemistry Chemical Physics}},
  number       = {{37}},
  pages        = {{19733--19747}},
  publisher    = {{Royal Society of Chemistry (RSC)}},
  title        = {{{A fast electrochemical quartz crystal microbalance (EQCM) evidences the presence of nanobubbles in alkaline water splitting}}},
  doi          = {{10.1039/d5cp02691a}},
  volume       = {{27}},
  year         = {{2025}},
}

@article{63244,
  abstract     = {{<jats:p>
            The Cauchy problem in 
            <jats:inline-formula>
              <jats:tex-math>\mathbb{R}^{n}</jats:tex-math>
            </jats:inline-formula>
             for the cross-diffusion system 
          </jats:p>
          <jats:p>
            <jats:disp-formula>
              <jats:tex-math>\begin{cases}u_{t} = \nabla \cdot (D(u)\nabla u) - \nabla\cdot (u\nabla v), \\ 0 = \Delta v +u,\end{cases}</jats:tex-math>
            </jats:disp-formula>
          </jats:p>
          <jats:p>
             is considered for 
            <jats:inline-formula>
              <jats:tex-math>n\ge 2</jats:tex-math>
            </jats:inline-formula>
             and under assumptions ensuring that 
            <jats:inline-formula>
              <jats:tex-math>D</jats:tex-math>
            </jats:inline-formula>
             suitably generalizes the prototype given by 
          </jats:p>
          <jats:p>
            <jats:disp-formula>
              <jats:tex-math>D(\xi)=(\xi+1)^{-\alpha}, \quad \xi\ge 0.</jats:tex-math>
            </jats:disp-formula>
          </jats:p>
          <jats:p>
             Under the assumption that 
            <jats:inline-formula>
              <jats:tex-math>\alpha&gt;1</jats:tex-math>
            </jats:inline-formula>
            , it is shown that for any 
            <jats:inline-formula>
              <jats:tex-math>r_{\star}&gt;0</jats:tex-math>
            </jats:inline-formula>
             and 
            <jats:inline-formula>
              <jats:tex-math>\delta\in (0,1)</jats:tex-math>
            </jats:inline-formula>
             one can find radially symmetric initial data from 
            <jats:inline-formula>
              <jats:tex-math>C_{0}^{\infty}(\mathbb{R}^{n})</jats:tex-math>
            </jats:inline-formula>
             such that the corresponding solution blows up within some finite time, and that this explosion occurs throughout certain spheres in an appropriate sense, with any such sphere being located in the annulus 
            <jats:inline-formula>
              <jats:tex-math>\overline{B}_{r_\star+\delta}(0)\setminus B_{(1-\delta)r_\star}(0)</jats:tex-math>
            </jats:inline-formula>
            .This is complemented by a result revealing that when 
            <jats:inline-formula>
              <jats:tex-math>\alpha&lt;1</jats:tex-math>
            </jats:inline-formula>
            , any finite-mass unbounded radial solution must blow up exclusively at the spatial origin.
          </jats:p>}},
  author       = {{Winkler, Michael}},
  issn         = {{1435-9855}},
  journal      = {{Journal of the European Mathematical Society}},
  publisher    = {{European Mathematical Society - EMS - Publishing House GmbH}},
  title        = {{{Can diffusion degeneracies enhance complexity in chemotactic aggregation? Finite-time blow-up on spheres in a quasilinear Keller–Segel system}}},
  doi          = {{10.4171/jems/1607}},
  year         = {{2025}},
}

@article{63344,
  abstract     = {{<jats:title>Abstract</jats:title>
          <jats:p>A Neumann-type initial-boundary value problem for <jats:disp-formula>
              <jats:alternatives>
                <jats:tex-math>$$\begin{aligned} \left\{ \begin{array}{l} u_{tt} = \nabla \cdot (\gamma (\Theta ) \nabla u_t) + a \nabla \cdot (\gamma (\Theta ) \nabla u) + \nabla \cdot f(\Theta ), \\ \Theta _t = D\Delta \Theta + \Gamma (\Theta ) |\nabla u_t|^2 + F(\Theta )\cdot \nabla u_t, \end{array} \right. \end{aligned}$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mtable>
                      <mml:mtr>
                        <mml:mtd>
                          <mml:mfenced>
                            <mml:mrow>
                              <mml:mtable>
                                <mml:mtr>
                                  <mml:mtd>
                                    <mml:mrow>
                                      <mml:msub>
                                        <mml:mi>u</mml:mi>
                                        <mml:mrow>
                                          <mml:mi>tt</mml:mi>
                                        </mml:mrow>
                                      </mml:msub>
                                      <mml:mo>=</mml:mo>
                                      <mml:mi>∇</mml:mi>
                                      <mml:mo>·</mml:mo>
                                      <mml:mrow>
                                        <mml:mo>(</mml:mo>
                                        <mml:mi>γ</mml:mi>
                                        <mml:mrow>
                                          <mml:mo>(</mml:mo>
                                          <mml:mi>Θ</mml:mi>
                                          <mml:mo>)</mml:mo>
                                        </mml:mrow>
                                        <mml:mi>∇</mml:mi>
                                        <mml:msub>
                                          <mml:mi>u</mml:mi>
                                          <mml:mi>t</mml:mi>
                                        </mml:msub>
                                        <mml:mo>)</mml:mo>
                                      </mml:mrow>
                                      <mml:mo>+</mml:mo>
                                      <mml:mi>a</mml:mi>
                                      <mml:mi>∇</mml:mi>
                                      <mml:mo>·</mml:mo>
                                      <mml:mrow>
                                        <mml:mo>(</mml:mo>
                                        <mml:mi>γ</mml:mi>
                                        <mml:mrow>
                                          <mml:mo>(</mml:mo>
                                          <mml:mi>Θ</mml:mi>
                                          <mml:mo>)</mml:mo>
                                        </mml:mrow>
                                        <mml:mi>∇</mml:mi>
                                        <mml:mi>u</mml:mi>
                                        <mml:mo>)</mml:mo>
                                      </mml:mrow>
                                      <mml:mo>+</mml:mo>
                                      <mml:mi>∇</mml:mi>
                                      <mml:mo>·</mml:mo>
                                      <mml:mi>f</mml:mi>
                                      <mml:mrow>
                                        <mml:mo>(</mml:mo>
                                        <mml:mi>Θ</mml:mi>
                                        <mml:mo>)</mml:mo>
                                      </mml:mrow>
                                      <mml:mo>,</mml:mo>
                                    </mml:mrow>
                                  </mml:mtd>
                                </mml:mtr>
                                <mml:mtr>
                                  <mml:mtd>
                                    <mml:mrow>
                                      <mml:mrow/>
                                      <mml:msub>
                                        <mml:mi>Θ</mml:mi>
                                        <mml:mi>t</mml:mi>
                                      </mml:msub>
                                      <mml:mo>=</mml:mo>
                                      <mml:mi>D</mml:mi>
                                      <mml:mi>Δ</mml:mi>
                                      <mml:mi>Θ</mml:mi>
                                      <mml:mo>+</mml:mo>
                                      <mml:mi>Γ</mml:mi>
                                      <mml:mrow>
                                        <mml:mo>(</mml:mo>
                                        <mml:mi>Θ</mml:mi>
                                        <mml:mo>)</mml:mo>
                                      </mml:mrow>
                                      <mml:msup>
                                        <mml:mrow>
                                          <mml:mo>|</mml:mo>
                                          <mml:mi>∇</mml:mi>
                                          <mml:msub>
                                            <mml:mi>u</mml:mi>
                                            <mml:mi>t</mml:mi>
                                          </mml:msub>
                                          <mml:mo>|</mml:mo>
                                        </mml:mrow>
                                        <mml:mn>2</mml:mn>
                                      </mml:msup>
                                      <mml:mo>+</mml:mo>
                                      <mml:mi>F</mml:mi>
                                      <mml:mrow>
                                        <mml:mo>(</mml:mo>
                                        <mml:mi>Θ</mml:mi>
                                        <mml:mo>)</mml:mo>
                                      </mml:mrow>
                                      <mml:mo>·</mml:mo>
                                      <mml:mi>∇</mml:mi>
                                      <mml:msub>
                                        <mml:mi>u</mml:mi>
                                        <mml:mi>t</mml:mi>
                                      </mml:msub>
                                      <mml:mo>,</mml:mo>
                                    </mml:mrow>
                                  </mml:mtd>
                                </mml:mtr>
                              </mml:mtable>
                            </mml:mrow>
                          </mml:mfenced>
                        </mml:mtd>
                      </mml:mtr>
                    </mml:mtable>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:disp-formula>is considered in a smoothly bounded domain <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$\Omega \subset \mathbb {R}^n$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mi>Ω</mml:mi>
                    <mml:mo>⊂</mml:mo>
                    <mml:msup>
                      <mml:mrow>
                        <mml:mi>R</mml:mi>
                      </mml:mrow>
                      <mml:mi>n</mml:mi>
                    </mml:msup>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula>, <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$n\ge 1$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mi>n</mml:mi>
                    <mml:mo>≥</mml:mo>
                    <mml:mn>1</mml:mn>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula>. In the case when <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$n=1$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mi>n</mml:mi>
                    <mml:mo>=</mml:mo>
                    <mml:mn>1</mml:mn>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula>, <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$\gamma \equiv \Gamma $$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mi>γ</mml:mi>
                    <mml:mo>≡</mml:mo>
                    <mml:mi>Γ</mml:mi>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula> and <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$f\equiv F$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mi>f</mml:mi>
                    <mml:mo>≡</mml:mo>
                    <mml:mi>F</mml:mi>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula>, this system coincides with the standard model for heat generation in a viscoelastic material of Kelvin-Voigt type, well-understood in situations in which <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$\gamma =const$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mi>γ</mml:mi>
                    <mml:mo>=</mml:mo>
                    <mml:mi>c</mml:mi>
                    <mml:mi>o</mml:mi>
                    <mml:mi>n</mml:mi>
                    <mml:mi>s</mml:mi>
                    <mml:mi>t</mml:mi>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula>. Covering scenarios in which all key ingredients <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$\gamma ,\Gamma ,f$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mi>γ</mml:mi>
                    <mml:mo>,</mml:mo>
                    <mml:mi>Γ</mml:mi>
                    <mml:mo>,</mml:mo>
                    <mml:mi>f</mml:mi>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula> and <jats:italic>F</jats:italic> may depend on the temperature <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$\Theta $$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mi>Θ</mml:mi>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula> here, for initial data which merely satisfy <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$u_0\in W^{1,p+2}(\Omega )$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:msub>
                      <mml:mi>u</mml:mi>
                      <mml:mn>0</mml:mn>
                    </mml:msub>
                    <mml:mo>∈</mml:mo>
                    <mml:msup>
                      <mml:mi>W</mml:mi>
                      <mml:mrow>
                        <mml:mn>1</mml:mn>
                        <mml:mo>,</mml:mo>
                        <mml:mi>p</mml:mi>
                        <mml:mo>+</mml:mo>
                        <mml:mn>2</mml:mn>
                      </mml:mrow>
                    </mml:msup>
                    <mml:mrow>
                      <mml:mo>(</mml:mo>
                      <mml:mi>Ω</mml:mi>
                      <mml:mo>)</mml:mo>
                    </mml:mrow>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula>, <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$u_{0t}\in W^{1,p}(\Omega )$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:msub>
                      <mml:mi>u</mml:mi>
                      <mml:mrow>
                        <mml:mn>0</mml:mn>
                        <mml:mi>t</mml:mi>
                      </mml:mrow>
                    </mml:msub>
                    <mml:mo>∈</mml:mo>
                    <mml:msup>
                      <mml:mi>W</mml:mi>
                      <mml:mrow>
                        <mml:mn>1</mml:mn>
                        <mml:mo>,</mml:mo>
                        <mml:mi>p</mml:mi>
                      </mml:mrow>
                    </mml:msup>
                    <mml:mrow>
                      <mml:mo>(</mml:mo>
                      <mml:mi>Ω</mml:mi>
                      <mml:mo>)</mml:mo>
                    </mml:mrow>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula> and <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$\Theta _0\in W^{1,p}(\Omega )$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:msub>
                      <mml:mi>Θ</mml:mi>
                      <mml:mn>0</mml:mn>
                    </mml:msub>
                    <mml:mo>∈</mml:mo>
                    <mml:msup>
                      <mml:mi>W</mml:mi>
                      <mml:mrow>
                        <mml:mn>1</mml:mn>
                        <mml:mo>,</mml:mo>
                        <mml:mi>p</mml:mi>
                      </mml:mrow>
                    </mml:msup>
                    <mml:mrow>
                      <mml:mo>(</mml:mo>
                      <mml:mi>Ω</mml:mi>
                      <mml:mo>)</mml:mo>
                    </mml:mrow>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula> with some <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$p\ge 2$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mi>p</mml:mi>
                    <mml:mo>≥</mml:mo>
                    <mml:mn>2</mml:mn>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula> such that <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$p&gt;n$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mi>p</mml:mi>
                    <mml:mo>&gt;</mml:mo>
                    <mml:mi>n</mml:mi>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula>, a result on local-in-time existence and uniqueness is derived in a natural framework of weak solvability.</jats:p>}},
  author       = {{Winkler, Michael}},
  issn         = {{0095-4616}},
  journal      = {{Applied Mathematics &amp; Optimization}},
  number       = {{2}},
  publisher    = {{Springer Science and Business Media LLC}},
  title        = {{{Rough Data in an Evolution System Generalizing 1D Thermoviscoelasticity with Temperature-Dependent Parameters}}},
  doi          = {{10.1007/s00245-025-10243-9}},
  volume       = {{91}},
  year         = {{2025}},
}

@inproceedings{63457,
  author       = {{Moritzer, Elmar and Völklein, Paul Leonhard}},
  booktitle    = {{Technomer 2025 29. Fachtagung}},
  isbn         = {{978-3-939382-17-1}},
  keywords     = {{Faserverstärkte Kunststoffe (FVK), mechanischens Fügen, Nieten, Organobleche}},
  title        = {{{Untersuchung des Erwärmverhaltens von Organoblechen mittels IR-Strahlung für das Fügen im Stempelnietverfahren}}},
  year         = {{2025}},
}

@techreport{63209,
  abstract     = {{Die DFG-Projekte AddFeRo-PM (406108415) und AddFeRo-SR (465089065) untersuchten die Potenziale des LB-PBF/M-Verfahrens zur Herstellung von Rotoren für unterschiedliche elektrische Maschinen. Im interdisziplinären Ansatz wurden Materialentwicklung und mechanische sowie elektromagnetische Optimierung verbunden. Im Projekt „AddFeRo-PM“ wurde der Rotor einer permanentmagneterregten Synchron- maschine (PMSM) untersucht. FeSi erwies sich als geeignete Legierung, konnte aber wegen Spannungsrissen nur bis zu 3 % Siliziumanteil (kurz: FeSi3) verarbeitet werden. Mechanische und elektromagnetische Untersuchungen ermöglichten eine 3D-Optimierung der Rotorgeometrie und -struktur. Der Demonstrator wurde additiv gefertigt und zeigt Leicht-baupotenziale sowie reduzierte Drehmomentwelligkeit. Im Folgeprojekt „AddFeRo-SR“ kam eine Hochtemperatur-Bauraumheizung (HTBH) zum Einsatz, die FeSi mit 6,5 % Siliziumanteil verarbeitbar machte, welches bessere elektro- magnetische Eigenschaften bietet. Sie wurde bei einer Synchron-Reluktanzmaschine (SynRM) getestet. Eine hybride Rotorfertigung erwies sich jedoch aufgrund von HTBH-Einschränkungen als ungeeignet, weshalb eine einteilige Fertigung mit FeSi3 umgesetzt wurde. Experimente bestätigten vergleichbare Betriebsergebnisse zur konventionellen Fertigung bei reduzierter Rotormasse. Zusätzlich wurde eine Methodik entwickelt, um additive Verfahren als Ergänzung zur konventionellen Fertigung zu integrieren. Beide Projekte zeigen das Potenzial additiver Fertigung für Leichtbau und Wirkungsgradsteigerung im Elektromaschinenbau und bieten wertvolle Grundlagen für industrielle Anwendungen.}},
  author       = {{Haase, Michael and Behrendt, Marius and Hengsbach, Florian and Kunnathully Sathees Kumar, Vinay and Magerkohl, Sebastian and Magyar, Balázs and Ponick, Bernd and Schaper, Mirko and Zimmer, Detmar}},
  keywords     = {{Additive Fertigung, Elektromotor, Leichtbau, Synchronmotor, DFG}},
  publisher    = {{Technische Informationsbibliothek}},
  title        = {{{Additive Fertigung im Elektromaschinenbau: Erforschung von Potentialen der additiven Fertigung in Rotoren permanentmagneterregter Synchronmaschinen}}},
  doi          = {{10.34657/26753}},
  year         = {{2025}},
}

@article{62713,
  abstract     = {{Periodically poled thin-film lithium niobate (TFLN) crystals are the fundamental building block for highly-efficient quantum light sources and frequency converters. The efficiency of these devices is strongly dependent on the interaction length between the light and the nonlinear material, scaling quadratically with this parameter. Nevertheless, the fabrication of long, continuously poled areas in TFLN remains challenging, the length of continuously poled areas rarely exceeds 10 mm. In this work, we demonstrate a significant progress in this field achieving the periodic poling of continuous poled areas of 70 mm length with a 3 μm poling period and a close to 50 % duty cycle. We compare two poling electrode design approaches to fabricate long, continuous poled areas. The first approach involves the poling of a single, continuous 70 mm long electrode. The second utilize a segmented approach including the poling of more than 20 individual sections forming together a 70 mm long poling area with no stitching errors. While the continuous electrode allows for faster fabrication, the segmented approach allows to individually optimize the poling resulting in less duty cycle variation. A detailed analysis of the periodic poling results reveals that the results of both are consistent with previously reported poling outcomes for shorter devices. Thus, we demonstrate wafer-scale periodic poling exceeding chiplet-size without any loss in the periodic poling quality. Our work presents a key step towards highly-efficient, narrow-bandwidth and low-pump power nonlinear optical devices.}},
  author       = {{Bollmers, Laura and Spiegelberg, Noah and Rüsing, Michael and Eigner, Christof and Padberg, Laura and Silberhorn, Christine}},
  issn         = {{2192-8606}},
  journal      = {{Nanophotonics}},
  pages        = {{4761}},
  publisher    = {{Walter de Gruyter GmbH}},
  title        = {{{Segmented finger electrodes to optimize ultra-long continuous wafer-scale periodic poling in thin-film lithium niobate}}},
  doi          = {{10.1515/nanoph-2025-0461}},
  volume       = {{14}},
  year         = {{2025}},
}

@article{62654,
  abstract     = {{<jats:title>Abstract</jats:title>
                  <jats:p>
                    Cationic gold catalyzed acetylene hydrochlorination represents a classical landmark in eliminating global mercury pollution, but their sustainable implementation is hindered by acetylene‐dependence design criteria and high operating temperatures. Herein, a platform of carbon‐supported single‐atoms Au catalysts (Au/BC and Au/NC) with polarized charge characteristics are developed via engineering Au sites with hosted B, N configurations. The negatively charged Au/BC catalyst unlocks the low‐temperature inactivity (413–423K) of the Au/NC catalyst while exhibiting superior catalytic performance in the 433–473K operating temperature range. We confirm that the classical scaling relationships on acetylene can be broken by narrowing the adsorption capacity between acetylene and HCl on Au
                    <jats:sup>δ⁻</jats:sup>
                    sites via facilitating the back‐donation of
                    <jats:italic>d</jats:italic>
                    electrons into the antibonding orbitals of acetylene. Prolonging the durability of Au catalysts is achieved through preceding an additional robust Au
                    <jats:sup>δ⁻</jats:sup>
                    → Au
                    <jats:sup>δ⁺</jats:sup>
                    cycle prior to the classic Au
                    <jats:sup>δ⁺</jats:sup>
                    → Au
                    <jats:sup>0</jats:sup>
                    route. This work opens a promising avenue for low temperature vinyl chloride production.
                  </jats:p>}},
  author       = {{Li, Chun and Liu, Ruoting and Zhang, Zilong and Zuo, Fangmin and Jiang, Tingting and Zhang, Haifeng and Wang, Bolin and Lopez Salas, Nieves}},
  issn         = {{1433-7851}},
  journal      = {{Angewandte Chemie International Edition}},
  number       = {{29}},
  publisher    = {{Wiley}},
  title        = {{{Engineering Charge Polarized Au Sites for Low‐Temperature Acetylene Hydrochlorination}}},
  doi          = {{10.1002/anie.202501370}},
  volume       = {{64}},
  year         = {{2025}},
}