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Correlations were established between the hyperfine field distribution around the Fe atoms, the multiferroic properties, and the high magnetoelectric coefficient in BaTiO-BiFeO multilayer stacks with variable BiFeO single layer thickness, down to 5 nm. Of key importance in this study was the deposition of Fe - enriched BiFeO, which enhances the sensitivity of conversion electron Mössbauer spectroscopy by orders of magnitude. The magnetoelectric coefficient α reaches a maximum of 60.2 V cm Oe at 300 K and at a DC bias field of 2 Tesla for a sample of 15 × (10 nm BaTiO-5 nm BiFeO) and is one of the highest values reported so far. Interestingly, the highest α is connected to a high asymmetry of the hyperfine field distribution of the multilayer composite samples. The possible mechanisms responsible for the strong magnetoelectric coupling are discussed.
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http://dx.doi.org/10.1039/c8nr00430g | DOI Listing |
Inorg Chem
August 2025
Department of Chemistry, School of Natural Sciences, University of Manchester, Oxford Road, Manchester M13 9PL, U.K.
Slow magnetic relaxation in monometallic single-molecule magnets containing Kramers ions in the lanthanide series are reasonably well understood. However, less work has been performed on the non-Kramers ions of the series, especially in the presence of hyperfine coupling between nuclear and electronic spins. Here we perform a thorough characterization of the relaxation properties of [TbPc][NBu], in zero and nonzero magnetic fields.
View Article and Find Full Text PDFNat Phys
June 2025
Sussex Centre for Quantum Technologies, University of Sussex, Brighton, UK.
Hyperfine energy levels in trapped ions offer long-lived spin states. In addition, the motion of these charged particles couples strongly to electric field perturbations. These characteristics make trapped ions attractive platforms for the quantum sensing of electric fields.
View Article and Find Full Text PDFOpt Express
February 2025
Trap loss spectroscopy, based on fluorescence detection, provides a real-time measurement technique that is advantageous for ultra-cold atomic systems, to monitor the interaction between microwave fields and Rydberg atoms. By employing the polarization combinations of excitation lasers and microwave fields, we achieve trap loss spectroscopy of multi-path transitions in magnetic Rydberg hyperfine states and observe Zeeman broadening. The contributions of laser power, Zeeman effect, and collision effects to the broadening of the trap loss spectrum were comprehensively analyzed.
View Article and Find Full Text PDFPhys Rev Lett
July 2025
Eötvös Loránd University, ELTE, Institute of Chemistry, Pázmány Péter sétány 1/A, 1117 Budapest, Hungary.
Rovibrational energies, wave functions, and Raman transition moments are reported for the lowest-energy states of the H_{3}^{+} molecular ion including the magnetic couplings of the proton spins and molecular rotation in the presence of a weak external magnetic field. The rovibrational-hyperfine-Zeeman Hamiltonian matrix is constructed and diagonalized using the rovibrational eigenstates and the proton spin functions. The developed methodology can be used to compute hyperfine-Zeeman effects also for higher-energy rovibrational excitations of H_{3}^{+} and other closed-shell polyatomic molecules.
View Article and Find Full Text PDFJ Chem Theory Comput
August 2025
Department of Chemistry, University of Copenhagen, Universitetsparken 5, DK-2100 Copenhagen Ø, Denmark.
We present the first implementation and computation of electron spin resonance isotropic hyperfine coupling constants (HFCs) on a quantum hardware. As illustrative test cases, we compute the HFCs for the hydroxyl radical (OH), nitric oxide (NO), and triplet hydroxyl cation (OH). Our approach integrates the qubit-ADAPT method with unrestricted orbital optimization in an active space framework.
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