Leschke was a research (and teaching) assistant to Ludwig Tewordt (1926–2016) at the Universität Hamburg, to Uwe Brandt at the Universität Dortmund, to Herbert Wagner (born 1935) at the Forschungszentrum Jülich (then: KFA Jülich), and to Richard Bausch (born 1935) at the [Heinrich-Heine–]Universität Düsseldorf (HHU) before he became a professor there in 1982 and at the FAU in 1983. In 1987, he was a guest professor at the University of Georgia, Athens (UGA) with host David P. Landau (born 1941). In 2004, he organized the workshop "Mathematics and physics of disordered systems" jointly with Michael Baake, Werner Kirsch, and Leonid A. Pastur at the Mathematisches Forschungsinstitut Oberwolfach (MFO), Germany.[4] In 2017, he organized the workshop "Fisher–Hartwig asymptotics, Szegő expansions, and applications to statistical physics" jointly with Alexander V. Sobolev and Wolfgang Spitzer at the American Institute of Mathematics (AIM), then located in San Jose, California.[5] From 1998 to 2011 Leschke belonged to the advisory board of the Annalen der Physik[6], then edited by Ulrich Eckern (born 1952) at the Universität Augsburg.[3]
Notable doctoral students of Leschke include Peter Müller[7] (born 1967) and Simone Warzel (born 1973). The first one is professor of mathematics at the Ludwig-Maximilians-Universität (LMU) in Munich and dean of the Faculty of Mathematics, Informatics, and Statistics (2021–2025). The second one is professor of mathematics at the Technische Universität München (TUM) in Garching near Munich.[8]
Leschke's research publications listed below all refer to properties of non-relativistic quantum systems which are modeled by some Hamiltonian, that is, by some self-adjoint operator on Hilbert space representing the total energy of the system, possibly depending on random variables simulating disorder. In the publications from 2000 to 2017 the Hamiltonian is of Schrödinger type, that is, an operator for the sum of the kinetic and potential energy of "point-like" particles in Euclidean space. The two publications with Kurt Broderix (1962–2000) extend previously known continuity properties of the corresponding one-parameter Schrödinger semi-group (or Gibbs operator for different temperatures) to rather general magnetic fields and to (random) potential fields possibly leading to unbounded semi-groups; by suitably extending the Feynman–Kac formula and using the diamagnetic inequality.[9] The other three publications from 2000 to 2004 consider the case of a single particle subject to a constant magnetic field and a random potential field. For a Poissonian field with positive single-impurity potential U the low-energy behavior of the integrated (or cumulative) density of states is derived, depending on the range of U. For a Gaussian random field (without an underlying lattice structure) the first proofs are given for the existence of the density of states and of Anderson localization in multi-dimensional continuous space.[10][11] The publications in 2014 and 2017 refer to the case of many non-interacting particles which obey Fermi–Dirac statistics. For the corresponding ideal Fermi gas in thermodynamic equilibrium they contain the first rigorous results on the asymptotic growth of its quantum Rényi entropies of (spatial) entanglement at arbitrary temperature.[12][13] These results have served as a standard of comparison for approximate arguments and/or numerical methods to better understand the correlations in many-fermion systems with interaction.[14][15] The publications in 2021 are among the first ones providing rigorous results on quantum versions of the classic(al) Sherrington–Kirkpatrick spin-glass model. In particular, they prove for the first time the existence of a phase transition (related to spontaneous replica-symmetry breaking) if the temperature and the strength of the "transverse" magnetic field are low enough.[16] The publication in 2023 illuminates this phase transition's relevance to the quantum-annealing algorithm in computer science.[17][18][19]
Leschke, H.; Sobolev, A.V.; Spitzer, W. (2017). "Trace formulas for Wiener-Hopf operators with applications to entropies of free fermionic equilibrium states". J. Funct. Anal. 273 (3): 1049–1094. arXiv:1605.04429. doi:10.1016/j.jfa.2017.04.005.
Broderix, K.; Leschke, H.; Müller, P. (2004). "Continuous integral kernels for unbounded Schrödinger semigroups and their spectral projections". J. Funct. Anal. 212 (2): 287–323. arXiv:math-ph/0209020. doi:10.1016/j.jfa.2004.01.009.
Hupfer, T.; Leschke, H.; Müller, P.; Warzel, S. (2001). "The absolute continuity of the integrated density of states for magnetic Schrödinger operators with certain unbounded random potentials". Commun. Math. Phys. 221: 229–254. arXiv:math-ph/0105046. doi:10.1007/s002200100467.
^Baake, M.; Kirsch, W.; Leschke, H.; Pastur, L. (2004). "Mathematics and physics of disordered systems". OWR. 1 (2): 1167–1232. doi:10.4171/OWR/2004/22.
^Lőrinczi, J.; Hiroshima, F.; Betz, V. (2022). Feynman–Kac-Type Theorems and Gibbs Measures on Path Space – Volume 1 (2nd ed.). De Gruyter. p. 532. ISBN978-3-11-033004-5.
^Chulaevsky, V.; Suhov, Y. (2014). Multi-scale Analysis for Random Quantum Systems with Interaction. Birkhäuser. p. 249. ISBN978-1-49-393952-7.
^Aizenman, M.; Warzel, S. (2015). Random Operators–Disorder Effects on Quantum Spectra and Dynamics. American Mathematical Society. p. 115. ISBN978-1-4704-1913-4.
^Leschke, H.; Sobolev, A.V.; Spitzer, W. (2016). "Large-scale behaviour of local and entanglement entropy of the free Fermi gas at any temperature". Journal of Physics A: Theoretical and Mathematical. 49 (30) 30LT04: 9pp. arXiv:1501.03412. Bibcode:2016JPhA...49DLT04L. doi:10.1088/1751-8113/49/30/30LT04.
^Leschke, H.; Sobolev, A.V.; Spitzer, W. (2022). "Rényi entropies of the free Fermi gas in multi-dimensional space at high temperature". In Basor, E.; Böttcher, A.; Erhardt, T.; Tracy, C.A. (eds.). Toeplitz Operators and Random Matrices – In Memory of Harold Widom. Cham: Birkhäuser/Springer Nature. pp. 477–508. arXiv:2201.11087. doi:10.1007/978-3-031-13851-5_21.