The effect of magnetic ions and disorder on superconducting beta ''-(BEDT-TTF)(4)[(H3O)M(C2O4)(3)]center dot C6H5NO2 salts, where M = Ga and Cr

J PHYS IV 114 (2004) 285-287

Authors:

AF Bangura, AI Coldea, A Ardavan, J Singleton, A Akutsu-Sato, H Akatsu, P Day

Abstract:

We report in magnetotransport measurements performed in magnetic fields of up to 33 T and at low temperatures (0.45 K

Fermi-surface topology and the effects of intrinsic disorder in a class of charge-transfer salts containing magnetic ions: β″-(BEDT-TTF)4[(H3O)M(C2O4)3]Y (M = Ga, Cr, Fe; Y = C5H5N)

Physical Review B - Condensed Matter and Materials Physics 69:8 (2004)

Authors:

AI Coldea, AF Bangura, J Singleton, A Ardavan, A Akutsu-Sato, H Akutsu, SS Turner, P Day

Abstract:

We report high-field magnetotransport measurements on β″-(BEDT-TTF)4[(H3O)M(C2O4)3]Y, where M = Ga, Cr, and Fe and Y = C5H5N. We observe similar Shubnikov-de Haas oscillations in all compounds, attributable to four quasi-two-dimensional Fermi-surface pockets, the largest of which corresponds to a cross-sectional area 8.5% of the Brillouin zone. The cross-sectional areas of the pockets are in agreement with the expectations for a compensated semimetal, and the corresponding effective masses are me, rather small compared to those of other BEDT-TTF salts. Apart from the case of the smallest Fermi-surface pocket, varying the M ion seems to have little effect on the overall Fermi-surface topology or on the effective masses. Despite the fact that all samples show quantum oscillations at low temperatures, indicative of Fermi liquid behavior, the sample and temperature dependence of the interlayer resistivity suggest that these systems are intrinsically inhomogeneous. It is thought that intrinsic tendency to disorder in the anions and/or the ethylene groups of the BEDT-TTF molecules leads to the coexistence of insulating and metallic states at low temperatures. A notional phase diagram is given for the general family of β″-(BEDT-TTF)4[(H3O)M(C2O4)3]Y salts. © 2004 The American Physical Society.

Structural and Magnetic Properties of Polypyrrole Nanocomposites

Molecular Crystals and Liquid Crystals Taylor & Francis 417:1 (2004) 235-243

Authors:

R Turcu, I Peter, O Pana, L Giurgiu, N Aldea, B Barz, MN Grecu, A Coldea

Non-adiabatic small polaron hopping in the n = 3 ruddlesden-popper compound Ca4Mn3O10

Journal of Physics Condensed Matter 15:40 (2003) 6817-6833

Authors:

J Lago, PD Battle, MJ Rosseinsky, AI Coldea, J Singleton

Abstract:

Magnetotransport properties of the compound Ca4Mn3 O10 are interpreted in terms of activated hopping of small magnetic polarons in the non-adiabatic regime. Polarons are most probably formed around Mn3+ sites created by oxygen sub-stoichiometry. The application of an external field reduces the size of the magnetic contribution to the hopping barrier and thus produces an increase in the conductivity. We argue that the change in the effective activation energy around TN is due to the crossover to variable range hopping conduction as antiferromagnetic order sets in.

Synthesis and characterisation of Sr1.2Nd0.8Mn0.6Rh0.4O4

Journal of Materials Chemistry 13:5 (2003) 1166-1172

Authors:

DJ Gallon, PD Battle, SJ Blundell, AI Coldea, MJ Rosseinsky, C Steer

Abstract:

A polycrystalline sample of Sr1.2Nd0.8Mn0.6Rh0.4O4 has been synthesised and characterised by neutron diffraction, dc magnetometry, muon spectroscopy and magnetotransport measurements. Ir is an n = 1 member of the Ruddlesden-Popper (RP) An + 1BnO3n + 1 family, having tetragonal (I4/mmm) symmetry [a = 3.86418(6), c = 12.4414(2) Å]. Rh and Mn cations are disordered over the six-coordinate sites within the perovskite layers of the RP structure and the A sites are occupied by a disordered distribution of Nd and Sr. In contrast to the analogous compound Sr1.2La 0.8Mn0.6Rh0.4O4, which showed long range ferromagnetic ordering in an applied field ar 2 K, a spin-glass transition was observed ar 16 K for the Nd-containing compound. No long range magnetic order was observed ar 2 K. A maximum magnetoresistance of ∼ 30% in a 140 kOe field was found at 125 K.