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Extracting the Hamiltonian parameters of nanoscale quantum magnets from experimental measurements is a significant challenge in quantum matter. Here we establish a machine learning strategy to extract the parameters of a spin Hamiltonian from inelastic spectroscopy with scanning tunneling microscopy, and we demonstrate this methodology experimentally with an artificial nanoscale molecular magnet based on cobalt phthalocyanine (CoPC) molecules on NbSe. We show that this technique allows us to extract the Hamiltonian parameters of a quantum magnet from the differential conductance, including the substrate-induced spatial variation of the exchange couplings. Our methodology leverages a machine learning algorithm trained on exact quantum many-body simulations with tensor networks of finite quantum magnets, leading to a methodology that predicts the Hamiltonian parameters of CoPC quantum magnets of arbitrary size. Our results demonstrate how quantum many-body methods and machine learning enable us to learn a microscopic description of nanoscale quantum many-body systems with scanning tunneling spectroscopy.
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http://dx.doi.org/10.1021/acs.nanolett.5c02502 | DOI Listing |
J Phys Chem A
September 2025
Department of Chemistry, University of Wisconsin-Madison, Madison, Wisconsin 53706, United States.
The rotational spectra and analysis of the two lowest-energy vibrationally excited states, ν (A', 126 cm, MP2) and ν (A″, 133 cm, MP2), of -1-cyano-1,3-butadiene from 130 to 375 GHz is presented. The state symmetries allow and type Coriolis coupling, the effects of which are observed due to the close energy spacing of these states. A combined total of 6744 transitions were modeled (σ < 60 kHz) with a partial-octic two-state A-reduced Hamiltonian including eight coupling parameters (, , , , , , , and ).
View Article and Find Full Text PDFDalton Trans
September 2025
Department of Chemistry, Jadavpur University, Kolkata-700032, India.
A series of homometallic tetranuclear Ln complexes, [Ln(μ-OH){pyC(OH)O}(OCCMe)] [{pyC(OH)O} = monoanionic -diol form of di-2-pyridyl ketone; Ln = Nd (1), Eu (2), Tb (3), Dy (4), Er (5) and Yb (6)], have been synthesized and characterized. The asymmetric unit of each of the tetranuclear derivatives comprises the dinuclear motif, [Ln(μ-OH){pyC(OH)O}(OCCMe)]. The core structure of this Ln family possesses two homometallic structural subunits, LnIII3O, which are further connected through the bridging μ-OH ligands.
View Article and Find Full Text PDFSci Rep
September 2025
Laboratoire Charles Coulomb (L2C), Univ. Montpellier, CNRS, Montpellier, France.
The cooperative binding of molecular agents onto a substrate is pervasive in living systems. To study whether a system shows cooperativity, one can rely on a fluctuation analysis of quantities such as the number of substrate-bound units and the residence time in an occupancy state. Since the relative standard deviation from the statistical mean monotonically decreases with the number of binding sites, these techniques are only suitable for small enough systems, such as those implicated in stochastic processes inside cells.
View Article and Find Full Text PDFEntropy (Basel)
August 2025
Departamento de Física, Universidade Estadual Paulista (UNESP), Av. 24A, 1515, São Paulo 13506-900, SP, Brazil.
We explore the concept of scaling invariance in a type of dynamical systems that undergo a transition from regularity to chaos. The systems are described by a two-dimensional, nonlinear mapping that preserves the area in the phase space. The key variables are the action and the angle, as usual from Hamiltonian systems.
View Article and Find Full Text PDFEntropy (Basel)
August 2025
Department of Physics, College of Science, Imam Mohammad Ibn Saud Islamic University (IMSIU), P.O. Box 90950, Riyadh 11623, Saudi Arabia.
In this work, we investigate the quantum coherence and purity in hydrogen atoms under dissipative dynamics, with a focus on the hyperfine structure states arising from the electron-proton spin interaction. Using the Lindblad master equation, we model the time evolution of the density matrix of the system, incorporating both the unitary dynamics driven by the hyperfine Hamiltonian and the dissipative effects due to environmental interactions. Quantum coherence is quantified using the L1 norm and relative entropy measures, while purity is assessed via von Neumann entropy, for initial states, including a maximally entangled Bell state and a separable state.
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