Collaborative Research Center 360
Constrained Quantum Matter
Less is more!
We use carefully chosen constraints to design and
manipulate quantum states in solids, seeking to create new quantum
materials and explore conceptual challenges from quantum information
theory to non-equilibrium physics.
Our outreach project in Augsburg is looking for a motivated student for a Hiwi position!
Our annual Retreat Meeting is coming up!
Frank Pollmann awarded with the Gottfried Wilhelm Leibniz prize 2026
In 2026, another member of the TRR360, Frank Pollmann from the Technical University Munich, is awarded with the Gottfried Wilhelm Leibniz prize 2026 which is handed out by the German Research Foundation (DFG). He will be given this prestigious prize in March 2026 for his work on statistical mechanics of many-body systems and their link to quantum information theory. More details can be found here.
2025 James C. McGroddy Prize awarded to Hidenori Takagi
We are very proud to announce that one member of the TRR 360, Hidenori Tagaki from the MPI for solid-state research in Stuttgart, will be awarded with the 2025 James C. McGroody Prize for New Materials. He is honoured “for seminal theoretical and experimental research, materials design and discoveries that pioneered the exploration of novel forms of topological quantum matter in spin-orbit assisted Mott insulators realized in transition metal oxides”. More information can be found here. The prize will be presented in March 2025.
Next events
Recent Articles
Kollar, M.; Dutta, A. (2026), arXiv: 2611.12859 datadoi: 10.5281/zenodo.24079060. @unpublished{kollar2026hiddensymmetryoperatorsasymmetric,The asymmetric quantum Rabi model, a two-level system with splitting Δ and bias ϵ coupled with strength g to a boson mode, has level crossings when ϵ is an integer multiple N of the mode frequency. They are due to a hidden symmetry operator J, for which no general formula has been available. Here we obtain J in closed form for every N. We find that J is given by the parity of the symmetric model times the continuant (ordered tridiagonal determinant) of N first-order operators, which are the Hamiltonians at the intermediate biases N−1,N−3,…,1−N minus a common number operator. The symmetry is thus a staircase of N bias steps that closes on the mirror image of the model precisely at integer bias. The proof uses induction on two commutation relations. The same relations hold in the asymmetric two-photon and two-mode models, written with the generators of su(1,1), so that the same continuant gives their symmetry operators for every order, previously known only for the lowest ones. We also relate the closed formula for J to the known recursion relations for its coefficients and give their terms of lowest order in Δ explicitly. |
Littlehales, M. T.; Bauer, A.; Bartkowiak, M.; Zolliker, M.; White, J. S.; Pfleiderer, C. In-situ azimuthal sample rotation within a horizontal-field cryomagnet for small-angle neutron scattering Unpublished (2026), arXiv:2611.05159. @unpublished{littlehalesInsituAzimuthalSample2026,We present an in-situ azimuthal rotation stage for small-angle neutron scattering measurements. The stage provides an azimuthal rotation range of 315∘ about the stage normal. At the reference sample-stick orientation, the stage normal is parallel to the incident neutron beam, so that the sample rotates in the plane perpendicular to the beam. Combined with a sample stick rotation about a second, orthogonal axis, the stage provides control of the magnetic-field direction relative to the crystal axes, while the field remains fixed in the laboratory frame. For a 5 mm diameter incident beam, sample-stick rotations of approximately ±315∘ are accessible with negligible additional attenuation from the holder. The commercial rotator is specified for operation between 1 and 373 K and in magnetic fields up to 35 T, making the stage nominally compatible with the full temperature (1.8 to 320 K) and field (0 to 6.8 T) ranges of the used cryomagnet. As a working example, we characterize its performance on a spherical single crystal of MnSi between 20 and 35 K and in fields up to 183 mT, observing local sample heating during operation of ∼20 mK per 5∘ step. We illustrate the design considerations behind the holder construction, with specific notes for mounting spherical samples, and discuss the resulting performance and limitations. |
Wiedemann, B.; Causer, G. L.; Chacon, A.; Zhang, S. L.; Khaydukov, Y.; Hesjedal, T.; Soltwedel, O.; Keller, T.; Mühlbauer, S.; Adams, T.; Halder, M.; Pfleiderer, C.; Böni, P. Reciprocal space mapping of magnetic order in thick epitaxial MnSi films Journal Article Phys. Rev. B 114, 254401 (2026). @article{wiedemannReciprocalSpaceMapping2026,We report near-surface small-angle neutron scattering (NS-SANS) and complementary off-specular neutron reflectometry (OSR) of the magnetic order in a single-crystalline epitaxial MnSi film grown on Si(111) in the thick-film limit. Providing a means of direct reciprocal space mapping, NS-SANS and OSR reveal one-dimensional magnetic modulations perpendicular to the film surface under magnetic fields parallel and perpendicular to the film surface, where additional polarized neutron reflectometry (PNR) and magnetization measurements are in excellent agreement with the literature. Regardless of the field orientation, our data do not suggest the presence of more complex spin textures, notably the formation of skyrmions. This observation establishes a distinct contrast to bulk MnSi thinned to similar nanoscale thicknesses, in which a skyrmion lattice dominates the phase diagram under perpendicular fields. Extended x-ray absorption fine structure measurements suggest that small shifts of the Si positions within the unstrained unit cell of the film control the magnetic state, representing the main structural difference between epitaxial and thinned bulk MnSi. |
Dutta, A.; Kollar, M. A universal gauge structure in the photon content of light-matter systems Unpublished (2026), arXiv: 2610.40446. @unpublished{dutta2026universalgaugestructurephoton,After truncating the matter Hilbert space of a single-mode light-matter model, gauge transformations leave the spectrum invariant whereas the ground-state photon number is gauge dependent, hence, its meaning remains disputed. We show that this gauge dependence obeys an exact algebraic law whenever the gauge transformation acts as a displacement of the field coupled to a matter operator G. Namely, the ground-state photon number is a quadratic polynomial in the gauge parameter λ, ⟨a†a⟩λ = ⟨a†a⟩0 + Cλ + Qλ2. Here the coefficients are the correlator C=⟨Gp⟩ of G and the field momentum p, and Q=⟨G2⟩. Its minimum over all gauges is naturally gauge-invariant, and for the quantum Rabi model it is determined by the ground-state energy alone. We show that it is strictly positive for the quantum Rabi and Dicke models with level splitting, so that a residual photon content survives in every gauge. At weak coupling the gauge of minimal photon number is the Jaynes-Cummings gauge, and for the Dicke model it remains so at all couplings in the thermodynamic limit. |
Koller, E.; Leeb, V.; Perkins, N. B.; Knolle, J. Raman Circular Dichroism and Quantum Geometry of Chiral Quantum Spin Liquids Journal Article Phys. Rev. B 114, (2026), datadoi: 10.5281/zenodo.14946046. @article{kollerRamanCircularDichroism2026,We show that the quantum geometry of fractionalized spin excitations in Mott-insulating quantum spin liquids (QSLs) gives rise to a finite Raman circular dichroism (RCD) signal. We identify conditions under which the Loudon-Fleury framework, where light modulates the underlying exchange interactions, and the light-matter-coupling approach, where the effective vector potential couples directly to the spinon bands, yield equivalent Raman vertices for the fractionalized quasiparticles. Using the latter, we derive an analytical decomposition of the RCD into different quantum geometric contributions. This reveals the sensitivity of the RCD to the underlying structure of the wave functions and the handedness of the excitations, rather than a nonzero Chern number of spinon excitations. To illustrate this, we apply our approach to two examples, the Kitaev honeycomb model in a magnetic field and a parton mean-field state of the chiral QSL on the triangular lattice. |
Impressions from past events








































The research programme
We seek to design and utilize new quantum states by taking advantage of the recently developed capability to tailor electron systems in complex materials through a variety of complementary constraints, focusing on spin-momentum locking, gauge structures of interacting spin systems, and kinetic constraints.
News
Here you can find all the important news around the project ConQuMat: recent publication, internal events for project members and opening for various positions.
Outreach - Öffentlichkeitsarbeit
Dive with us into the fascinating world of quantum matter! (science communication offers in German)
Es gibt viele Angebote, um die Forschung aus dem Projekt ConQuMat der Öffentlichkeit zugänglich zu machen. Egal ob durch einen Blog, Spiele oder Erlebnisveranstaltungen – tauchen Sie mit uns in die faszinierende Welt der Quantenmaterie ein!