Organic Transistors: Universal Magnetic Hall Circuit Based on Paired Spin Heterostructures (Adv. Electron. Mater. 6/2015)

Advanced Electronic Materials 1 (2016)

S Zhang, AA Baker, JY Zhang, G Yu, S Wang, T Hesjedal

Modulated spin helicity stabilized by incommensurate orbital density waves in a quadruple perovskite manganite

PHYSICAL REVIEW B 93 (2016) ARTN 180403

RD Johnson, DD Khalyavin, P Manuel, A Bombardi, C Martin, LC Chapon, PG Radaelli

Magnetic phase diagram of La2-xSrxCoO4 revised using muon-spin relaxation

PHYSICAL REVIEW B 93 (2016) ARTN 140406

RC Williams, F Xiao, T Lancaster, R De Renzi, G Allodi, S Bordignon, PG Freeman, FL Pratt, SR Giblin, JS Moeller, SJ Blundell, AT Boothroyd, D Prabhakaran

Structural, electronic, and magnetic investigation of magnetic ordering in MBE-grown CrxSb2-xTe3 thin films

EPL 115 (2016) ARTN 27006

LJ Collins-McIntyre, LB Duffy, A Singh, N-J Steinke, CJ Kinane, TR Charlton, A Pushp, AJ Kellock, SSP Parkin, SN Holmes, CHW Barnes, G Van der Laan, S Langridge, T Hesjedal

Transverse field muon-spin rotation measurement of the topological anomaly in a thin film of MnSi

Physical Review B: Condensed Matter and Materials Physics American Physical Society 93 (2016) 140412(R)

T Lancaster, F Xiao, Z Salman, IO Thomas, SJ Blundell, F Pratt, SJ Clark, T Prokscha, A Suter, SL Zhang, AA Baker, T Hesjedal

Coherent Magnetoelastic Domains in Multiferroic BiFeO_{3} Films.

Physical review letters 117 (2016) 177601-

N Waterfield Price, RD Johnson, W Saenrang, F Maccherozzi, SS Dhesi, A Bombardi, FP Chmiel, C-B Eom, PG Radaelli

The physical properties of epitaxial films can fundamentally differ from those of bulk single crystals even above the critical thickness. By a combination of nonresonant x-ray magnetic scattering, neutron diffraction and vector-mapped x-ray magnetic linear dichroism photoemission electron microscopy, we show that epitaxial (111)-BiFeO_{3} films support submicron antiferromagnetic domains, which are magnetoelastically coupled to a coherent crystallographic monoclinic twin structure. This unique texture, which is absent in bulk single crystals, should enable control of magnetism in BiFeO_{3} film devices via epitaxial strain.

Polarization memory in the nonpolar magnetic ground state of multiferroic CuFeO2

PHYSICAL REVIEW B 94 (2016) ARTN 144411

J Beilsten-Edmands, SJ Magorrian, FR Foronda, D Prabhakaran, PG Radaelli, RD Johnson

Magnetostriction-driven ground-state stabilization in 2H perovskites

PHYSICAL REVIEW B 94 (2016) ARTN 134404

DG Porter, MS Senn, DD Khalyavin, A Cortese, N Waterfield-Price, PG Radaelli, P Manuel, H-C zur-Loye, C Mazzoli, A Bombardi

Single crystal growth from separated educts and its application to lithium transition-metal oxides.

Scientific Reports 6 (2016) 35362-

F Freund, SC Williams, RD Johnson, R Coldea, P Gegenwart, A Jesche

Thorough mixing of the starting materials is the first step of a crystal growth procedure. This holds true for almost any standard technique, whereas the intentional separation of educts is considered to be restricted to a very limited number of cases. Here we show that single crystals of α-Li2IrO3 can be grown from separated educts in an open crucible in air. Elemental lithium and iridium are oxidized and transported over a distance of typically one centimeter. In contrast to classical vapor transport, the process is essentially isothermal and a temperature gradient of minor importance. Single crystals grow from an exposed condensation point placed in between the educts. The method has also been applied to the growth of Li2RuO3, Li2PtO3 and β-Li2IrO3. A successful use of this simple and low cost technique for various other materials is anticipated.

Free-standing millimetre-long Bi2Te3 sub-micron belts catalyzed by TiO2 nanoparticles.

Nanoscale research letters 11 (2016) 308-

P Schönherr, F Zhang, D Kojda, R Mitdank, M Albrecht, SF Fischer, T Hesjedal

Physical vapour deposition (PVD) is used to grow millimetre-long Bi2Te3 sub-micron belts catalysed by TiO2 nanoparticles. The catalytic efficiency of TiO2 nanoparticles for the nanostructure growth is compared with the catalyst-free growth employing scanning electron microscopy. The catalyst-coated and catalyst-free substrates are arranged side-by-side, and overgrown at the same time, to assure identical growth conditions in the PVD furnace. It is found that the catalyst enhances the yield of the belts. Very long belts were achieved with a growth rate of 28 nm/min. A ∼1-mm-long belt with a rectangular cross section was obtained after 8 h of growth. The thickness and width were determined by atomic force microscopy, and their ratio is ∼1:10. The chemical composition was determined to be stoichiometric Bi2Te3 using energy-dispersive X-ray spectroscopy. Temperature-dependent conductivity measurements show a characteristic increase of the conductivity at low temperatures. The room temperature conductivity of 0.20 × 10(5) S m (-1) indicates an excellent sample quality.

Magnetization dynamics and frustration in the multiferroic double perovskite Lu2MnCoO6

PHYSICAL REVIEW B 93 (2016) ARTN 134431

VS Zapf, BG Ueland, M Laver, M Lonsky, M Pohlit, J Mueller, T Lancaster, JS Moeller, SJ Blundell, J Singleton, J Mira, S Yanez-Vilar, M Antonia Senaris-Rodriguez

Ab initio cycloidal and chiral magnetoelectric responses in Cr2O3

PHYSICAL REVIEW B 94 (2016) ARTN 100405

N Tillack, JR Yates, PG Radaelli

One-Step SnO2 Nanotree Growth.

Chemistry (Weinheim an der Bergstrasse, Germany) 22 (2016) 13823-13825

P Schönherr, T Hesjedal

A comparison between Au, TiO2 and self-catalysed growth of SnO2 nanostructures using chemical vapour deposition is reported. TiO2 enables growth of a nanonetwork of SnO2 , whereas self-catalysed growth results in nanoclusters. Using Au catalyst, single-crystalline SnO2 nanowire trees can be grown in a one-step process. Two types of trees are identified that differ in size, presence of a catalytic tip, and degree of branching. The growth mechanism of these nanotrees is based on branch-splitting and self-seeding by the catalytic tip, facilitating at least three levels of branching, namely trunk, branch and leaf.

Magnetic phase diagram of La2−xSrxCoO4 revised using muon-spin relaxation

Physical Review B - Condensed Matter and Materials Physics American Physical Society (2016)

RC Williams, F Xiao, T Lancaster, R De Renzi, G Allodi, S Bordignon, PG Freeman, FL Pratt, SR Giblin, JS Moeller, SJ Blundell, AT Boothroyd, D Prabhakaran

On the temperature dependence of spin pumping in ferromagnet-topological insulator-ferromagnet spin valves

Results in Physics 6 (2016) 293-294

AA Baker, AI Figueroa, G van der Laan, T Hesjedal

Detailed crystallographic analysis of the ice VI to ice XV hydrogen ordering phase transition.

The Journal of chemical physics 145 (2016) 204501-

CG Salzmann, B Slater, PG Radaelli, JL Finney, JJ Shephard, M Rosillo-Lopez, J Hindley

The D2O ice VI to ice XV hydrogen ordering phase transition at ambient pressure is investigated in detail with neutron diffraction. The lattice constants are found to be sensitive indicators for hydrogen ordering. The a and b lattice constants contract whereas a pronounced expansion in c is found upon hydrogen ordering. Overall, the hydrogen ordering transition goes along with a small increase in volume, which explains why the phase transition is more difficult to observe upon cooling under pressure. Slow-cooling ice VI at 1.4 GPa gives essentially fully hydrogen-disordered ice VI. Consistent with earlier studies, the ice XV obtained after slow-cooling at ambient pressure is best described with P-1 space group symmetry. Using a new modelling approach, we achieve the atomistic reconstruction of a supercell structure that is consistent with the average partially ordered structure derived from Rietveld refinements. This shows that C-type networks are most prevalent in ice XV, but other structural motifs outside of the classifications of the fully hydrogen-ordered networks are identified as well. The recently proposed Pmmn structural model for ice XV is found to be incompatible with our diffraction data, and we argue that only structural models that are capable of describing full hydrogen order should be used.

Incommensurate counterrotating magnetic order stabilized by Kitaev interactions in the layered honeycomb alpha-Li2IrO3

PHYSICAL REVIEW B 93 (2016) ARTN 195158

SC Williams, RD Johnson, F Freund, S Choi, A Jesche, I Kimchi, S Manni, A Bombardi, P Manuel, P Gegenwart, R Coldea

Large Fermi Surface of Heavy Electrons at the Border of Mott Insulating State in NiS2

Scientific Reports 6 (2016)

S Friedemann, H Chang, MB Gamża, P Reiss, X Chen, P Alireza, WA Coniglio, D Graf, S Tozer, FM Grosche

Unconventional magnetism on a honeycomb lattice in alpha-RuCl3 studied by muon spin rotation

PHYSICAL REVIEW B 94 (2016) ARTN 020407

F Lang, PJ Baker, AA Haghighirad, Y Li, D Prabhakaran, R Valenti, SJ Blundell

Transverse field muon-spin rotation measurement of the topological anomaly in a thin film of MnSi

PHYSICAL REVIEW B 93 (2016) ARTN 140412

T Lancaster, F Xiao, Z Salman, IO Thomas, SJ Blundell, FL Pratt, SJ Clark, T Prokscha, A Suter, SL Zhang, AA Baker, T Hesjedal