Thermodynamic features and enthalpy relaxation in a metal-organic framework glass.

Physical chemistry chemical physics : PCCP 20:27 (2018) 18291-18296

Authors:

Chao Zhou, Malwina Stepniewska, Louis Longley, Christopher W Ashling, Philip A Chater, David A Keen, Thomas D Bennett, Yuanzheng Yue

Abstract:

In this work, we explore the thermodynamic evolution in a melt-quenched metal-organic framework glass, formed from ZIF-62 upon heating to the melting point (Tm), and subsequent enthalpy relaxation. The temperature dependence of the difference in Gibbs free energy between the liquid and crystal states of ZIF-62 in the temperature range from the glass transition temperature (Tg) to Tm is found to be weaker than those of other types of glasses, e.g., metallic glasses. Additionally, we find that the stretched exponent of the enthalpy relaxation function in the glass varies significantly (β = 0.44-0.76) upon changing the extent of sub-Tg annealing, compared to metallic and oxide glasses with similar Tgs, suggesting a high degree of structural heterogeneity. Pair distribution function results suggest no significant structural changes during the sub-Tg relaxation in ZIF-62 glass.

Coupling of magnetic order and charge transport in the candidate Dirac semimetal EuCd2As2

Physical review B: Condensed matter and materials physics American Physical Society 97:21 (2018) 214422

Authors:

MC Rahn, Jian R Soh, S Francoual, LSI Veiga, J Strempfer, J Mardegan, DY Yan, YF Guo, YG Shi, Andrew Boothroyd

Abstract:

We use resonant elastic x-ray scattering to determine the evolution of magnetic order in EuCd 2 As 2 below T N = 9.5 K, as a function of temperature and applied magnetic field. We find an A-type antiferromagnetic structure with in-plane magnetic moments, and observe dramatic magnetoresistive effects associated with field-induced changes in the magnetic structure and domain populations. Our ab initio electronic structure calculations indicate that the Dirac dispersion found in the nonmagnetic Dirac semimetal Cd 3 As 2 is also present in EuCd 2 As 2 , but is gapped for T < T N due to the breaking of C 3 symmetry by the magnetic structure.

Magnetic and electronic structure of the layered rare-earth pnictide EuCd$_2$Sb$_2$

(2018)

Authors:

J-R Soh, C Donnerer, KM Hughes, E Schierle, E Weschke, D Prabhakaran, AT Boothroyd

Monoclinic distortion, polarization rotation and piezoelectricity in the ferroelectric Na0.5Bi0.5TiO3

IUCrJ International Union of Crystallography 5:4 (2018) 417-427

Authors:

H Choe, J Bieker, N Zhang, Anthony M Glazer, PA Thomas, S Gorfman

Abstract:

The relationship between crystal structure and physical properties in the ferroelectric Na0.5Bi0.5TiO3 (NBT) has been of interest for the last two decades. Originally, the average structure was held to be of rhombohedral (R3c) symmetry with a fixed polarization direction. This has undergone a series of revisions, however, based on high-resolution X-ray diffraction, total neutron scattering, and optical and electron microscopy. The recent experimental findings suggest that the true average symmetry is monoclinic (space group Cc), which allows for a rotatable spontaneous polarization. Neither polarization rotation nor its potentially important real role in enhanced piezoelectricity is well understood. The present work describes an in situ investigation of the average monoclinic distortion in NBT by time-resolved single-crystal X-ray diffraction under external electric fields. The study presents a high-resolution inspection of the characteristic diffraction features of the monoclinic distortion – splitting of specific Bragg reflections – and their changes under a cyclic electric field. The results favour a model in which there is direct coupling between the shear monoclinic strain and the polarization rotation. This suggests that the angle of polarization rotation under a sub-coercive electric field could be 30° or more.

Liquid phase blending of metal-organic frameworks.

Nature communications 9:1 (2018) 2135

Authors:

Louis Longley, Sean M Collins, Chao Zhou, Glen J Smales, Sarah E Norman, Nick J Brownbill, Christopher W Ashling, Philip A Chater, Robert Tovey, Carola-Bibiane Schönlieb, Thomas F Headen, Nicholas J Terrill, Yuanzheng Yue, Andrew J Smith, Frédéric Blanc, David A Keen, Paul A Midgley, Thomas D Bennett

Abstract:

The liquid and glass states of metal-organic frameworks (MOFs) have recently become of interest due to the potential for liquid-phase separations and ion transport, alongside the fundamental nature of the latter as a new, fourth category of melt-quenched glass. Here we show that the MOF liquid state can be blended with another MOF component, resulting in a domain structured MOF glass with a single, tailorable glass transition. Intra-domain connectivity and short range order is confirmed by nuclear magnetic resonance spectroscopy and pair distribution function measurements. The interfacial binding between MOF domains in the glass state is evidenced by electron tomography, and the relationship between domain size and Tg investigated. Nanoindentation experiments are also performed to place this new class of MOF materials into context with organic blends and inorganic alloys.