Erratum: Splitting of the transition to the antiferroelectric state in PbZr0.95Ti0.05O3 into polar and antiferrodistortive components [Phys. Rev. B 88, 094107 (2013)]

Physical Review B American Physical Society (APS) 107:9 (2023) 099901

Authors:

F Cordero, F Craciun, F Trequattrini, C Galassi, PA Thomas, DS Keeble, AM Glazer

Tuning of Polar Domain Boundaries in Nonpolar Perovskite.

Advanced materials (Deerfield Beach, Fla.) 35:11 (2023) e2207665

Authors:

Zheyi An, Hiroko Yokota, Kyomaru Kurihara, Nozomu Hasegawa, Pavel Marton, Anthony Michael Glazer, Yoshiaki Uesu, Wei Ren, Zuo-Guang Ye, Marek Paściak, Nan Zhang

Abstract:

Domain boundaries in ferroic materials are found to have various physical properties not observed in the surrounding domains. Such differences can be enhanced and bring promising functionalities when centrosymmetric nonpolar materials encounter polar domain boundaries. In this work, a tunable polar domain boundary is discovered in an antiferroelectric single crystal. Under a small stress or electric field, the density, volume, and polarity of the boundaries are successfully controlled.

Formation of a meltable purinate metal-organic framework and its glass analogue.

Chemical communications (Cambridge, England) 59:6 (2023) 732-735

Authors:

Alice M Bumstead, Celia Castillo-Blas, Ignas Pakamorė, Michael F Thorne, Adam F Sapnik, Ashleigh M Chester, Georgina Robertson, Daniel JM Irving, Philip A Chater, David A Keen, Ross S Forgan, Thomas D Bennett

Abstract:

The chemistries that can be incorporated within melt-quenched zeolitic imidazolate framework (ZIF) glasses are currently limited. Here we describe the preparation of a previously unknown purine-containing ZIF which we name ZIF-UC-7. We find that it melts and forms a glass at one of the lowest temperatures reported for 3D hybrid frameworks.

Phase transition hysteresis at the antiferroelectric-ferroelectric boundary in PbZr1−xTixO3

Physical Review B American Physical Society (APS) 106:22 (2022) 224103

Authors:

Zheyi An, Shanshan Xie, Petr Ondrejkovic, Pavel Marton, Esther de Prado, Hiroko Yokota, Wei Ren, Zuo-Guang Ye, AM Glazer, Marek Paściak, Nan Zhang

Impact of mixed anion ordered state on the magnetic ground states of S=1/2 square-lattice quantum spin antiferromagnets, Sr2NiO3Cl and Sr2NiO3F

Physical Review Materials American Physical Society 6:11 (2022) 114404

Authors:

Y Tsujimoto, J Sugiyama, M Ochi, K Kuroki, P Manuel, Dd Khalyavin, I Umegaki, M Månsson, D Andreica, S Hara, T Sakurai, S Okubo, H Ohta, At Boothroyd, K Yamaura

Abstract:

The magnetic properties of the S=1/2 two-dimensional square-lattice antiferromagnets Sr2NiO3X (X=Cl, F) with the trivalent nickel ions in a low-spin state were studied by magnetic susceptibility, heat capacity, neutron powder diffraction, high-field electron spin resonance (ESR), muon spin rotation and relaxation (μ+SR) measurements, and density functional theory (DFT) calculations. Both oxyhalides are isostructural to an ideal quantum square-lattice antiferromagnet Sr2CuO2Cl2, but the chlorine/fluorine anion exclusively occupies an apical site in an ordered/disordered manner with an oxygen anion, resulting in the formation of highly distorted NiO5X octahedra with an off-center nickel ion. Magnetic susceptibility measurements revealed a remarkable difference between these two compounds: the magnetic susceptibility of Sr2NiO3Cl exhibited a broad maximum at approximately 35 K, which is typical of low-dimensional antiferromagnetic behavior. In contrast, the magnetic susceptibility of Sr2NiO3F exhibited spin-glass-like behavior below 12 K. No anomaly associated with long-range magnetic ordering was observed in the heat capacity, ESR, and neutron powder diffraction experiments. However, μ+SR measurements revealed the emergence of a static magnetic ordered state below TN=28K in Sr2NiO3Cl and a short-range magnetic state below TN=18K in Sr2NiO3F. The DFT calculations suggested that the unpaired electron occupied a d3z2-r2 orbital, and ferromagnetic couplings between the nearest-neighbor nickel spins were energetically favored. The mechanism of ferromagnetic superexchange interactions and the reason for the difference between the magnetic ground states in these nickel oxyhalides are discussed.