Quantum states of muons in fluorides

Phys. Rev. B American Physical Society 87 (2013) 121108-121108

Authors:

JS Möller, D Ceresoli, T Lancaster, N Marzari, SJ Blundell

Weak magnetic transitions in pyrochlore Bi2Ir2O7

(2013)

Authors:

PJ Baker, JS Moeller, FL Pratt, W Hayes, SJ Blundell, T Lancaster, TF Qi, G Cao

Orbital Approach to the Electronic Structure of Solids, by E. Canadell, M.-L. Doublet and C. Iung

Contemporary Physics Taylor & Francis 54:1 (2013) 56-57

Stripe disorder and dynamics in the hole-doped antiferromagnetic insulator La5/3Sr1/3CoO4

(2013)

Authors:

T Lancaster, SR Giblin, G Allodi, S Bordignon, M Mazzani, R De Renzi, PG Freeman, PJ Baker, FL Pratt, P Babkevich, SJ Blundell, AT Boothroyd, JS Moeller, D Prabhakaran

Antiferromagnetic ordering through a hydrogen-bonded network in the molecular solid CuF2(H2O)2(3-chloropyridine).

Chem Commun (Camb) 49:5 (2013) 499-501

Authors:

Saul H Lapidus, Jamie L Manson, Hyunsoo Park, Alexander J Clement, Saman Ghannadzadeh, Paul Goddard, Tom Lancaster, Johannes S Möller, Stephen J Blundell, Mark TF Telling, Jinhee Kang, Myung-Hwan Whangbo, John A Schlueter

Abstract:

CuF(2)(H(2)O)(2)(3-chloropyridine) possesses a five-coordinate Cu(2+) center with a slightly distorted trigonal bypyramidal coordination geometry. Strong intermolecular F···H-O hydrogen bonds enable the formation of 2D layers and provide the primary magnetic exchange path that leads to the stabilization of long-range antiferromagnetic (AFM) order below T(N) = 2.1 K.